优秀英文 blog

Surfer dude in a coffee machine may supersede the LHC

Luboš Motl’s Reference Frame - 周二, 2009-01-06 15:47

While the LHC is going to be restarted in June after a "catastrophic malfunction", as the journalists call the routine, expected, and mundane breakdown of a few magnets following a quench, you may have wondered that it is too large and expensive a machine. USD 9 billion is not a negligible amount of money. 

Can't the physicists design a somewhat cheaper gadget, one that is similar e.g. to a coffee machine?



Figure 1: A prototype of the new kind of an atom smasher. Image from Lawrence Berkeley National Labs (LBNL).

Nude Socialist and others describe a new design that is pretty close to that goal. Building on a 1979 paper by John Dawson (UCLA) and Toshiki Tajima (Austin), Wim Leemans et al. (LBNL) are constructing much cheaper devices based on powerful lasers.

A coffee machine heats up some water to get a plasma and a powerful laser creates mesoscopic waves that make electrons oscillate, or surf on the waves, and accelerate to potentially huge energies.



Figure 2: The wave effect of a high-intensity pulse laser. The same credits. Click the images to zoom in.

But don't expect any old-fashioned experimental particle physicists to be arrested for wasting the taxpayers' money any time soon. So far they only work on the acceleration to relatively small energies and dream about dozens of GeV in the electron beams. In the 2020s, they could get to hundreds of GeVs if the laser power gets really cheap and if they're lucky.

If that becomes the case, surfer dudes could be useful for high-energy physics, after all.

Best European Blog: a contest

Luboš Motl’s Reference Frame - 周二, 2009-01-06 05:12


Between now and January 12th (5 pm Boston time), click the image above every day and choose TRF (2nd column, 2nd row) or one of nine other attractive blogs that have been nominated as the best European blog. Boringly enough, I am not aware of any real "foes" in our European category.

Encourage your friends to objectively choose between TRF and the other interesting blogs, too.

Don't forget about the best science blog where Steve McIntyre and Anthony Watts will compete against Bad Astronomy and Real Climate, among six others.

Thanks to Eduardo for his nomination - and the same thanks for Rae Ann's and two more nominations in the science category where others have beaten us before the contest began. ;-)

Bonus: New Year Address

By the way, you may watch a peaceful Czech president Václav Klaus' New Year Address with a direct translation to (Cz)English by your humble correspondent.

Science Lesson: Creativity and pollution

Impropable Research - 周二, 2009-01-06 04:28

Today’s lesson teaches that a scientist can make great discoveries by being creative.

A new kind of scientific detective work has, reportedly, paid off bigtime in the field of environmental science.

Thousands of scientists labored for decades to identify the most dangerous sources of environmental pollution—but despite all their slow, careful measurement and experimentation, they failed to identify what we now learn is a major source of pollution. A January 5, 2009 Catholic News Service report explains:

The birth-control pill is causing “devastating” environmental damage and plays a role in rising male infertility rates, said the Vatican newspaper, L’Osservatore Romano…. Pedro Jose-Maria Simon-Castellvi, president of the Vatican-based World Federation of Catholic Medical Associations, wrote the article that appeared in the paper’s Jan. 4 edition.

The pill has created “devastating ecological effects from tons of hormones being released into the environment for years,” the article said.

Details have not yet been made public. Students (along with every environmental scientist in the world!) can now giddily await the day when Dr. Simon-Castelvi publishes a formal study, in a good science journal, giving details of how he achieved his breakthrough discovery.

(Thanks to investigator David Kessler for bringing this to our attention.)

Types of elementary particles

Luboš Motl’s Reference Frame - 周二, 2009-01-06 04:11

One of the main features of "progress" in theoretical physics is the unification of concepts and the emergence of tight links between previously unrelated concepts and assumptions. As this process continued (and continues), our theory were (and are) becoming more robust because they were (and are) built on a smaller number of independent assumptions.

This process is often misunderstood by the laymen who would often prefer the "progress" that invents or discovers completely new things that are unrelated to everything we have ever seen. Well, don't get me wrong, new effects and objects have to be sometimes discovered and science has to cover an ever larger set of phenomena. On the other hand, this is the "zoological" part of the progress in which new species are being constantly added. As soon as they are added, they are understood at a superficial level only.



The "philosophical" part of the progress that connects and unifies the old discoveries into an ever tighter network is more profound. This sort of development may be document by our perspective on the question what are the elementary particles in Nature. Modern quantum field theory describes pretty much all kinds of particles we know by the same formalism: the differences between types of particles that were previously viewed as "radically different" become either technicalities or different faces of the same underlying structure that inevitably follow as long as one understands this structure well.

In this text, I will describe different "iron curtains" that seem to separate "completely different" categories of particles in the minds of many people and explain the relationships between the individual "blocs". These relationships could be found by "pure thought" of sufficiently intelligent observers, at least in principle.

Particles vs waves

Since the early days of quantum mechanics, and even the old quantum theory, people knew that particles and waves were just two aspects of the same thing. Electromagnetic waves and similar objects that were historically identified as waves became a stream of particles such as photons. The energy carried by one quantum of energy always has to be proportional to "hf" where "h" is Planck's constant and "f" is the frequency. 

(It's easier to type "h" than "hbar" and "f" than "omega" here.)

On the other hand, objects first identified as particles, for example electrons, were found to exhibit wave-like behavior, including interference. All of them are described by wave functions (probability waves) that became a prototype of a quantum field later, when multiparticle theories were studied by the methods of the second quantization.

Why were the photons initially known as waves (and classical forces) while electrons were known as particles (that can be counted)? Well, it's because the photons are bosons which means that they like to be grouped with their identical friends in the same state. That's why there are usually many photons in the same state, "N", and this large number effectively becomes continuous which is why the collective probability wave describing the state becomes a classical wave, in this case an electromagnetic one.

On the other hand, electrons are fermions that have to obey Pauli's exclusion principle. That's why they can never be found in the same state as another particle of the same type and they can never give rise to coherent fields and long-range forces. One always has to observe them individually, and because the waves in their typical wave functions were much shorter than the resolution of the 19th century physicists (roughly than the atomic radius), people initially didn't know about their quantum/wave properties.

Bosons vs fermions

This discussion leads us to bosons and fermions. It may look like they are completely different types of animals. Bosons prefer to look like classical waves while fermions prefer to look like classical particles. However, when you describe them in the language of quantum field theory, this seemingly qualitative difference boils down to a single sign in which they differ.

Wave functions of bosons are symmetric under the exchange of the coordinates (and other quantum numbers) of pairs of identical particles,
psi(x,y) = +psi(y,x),
while wave functions of fermions are antisymmetric: they flip the sign:
psi(x,y) = -psi(y,x).
In terms of quantum fields, bosons are described by commuting quantum fields while fermions by the anticommuting ones. Anticommuting (Grassmannian) numbers are a bit counter-intuitive for the newbies but if you learn how to deal with all aspects of quantum theory properly, you will see that the Grassmannian numbers work as well as the ordinary, commuting numbers for all the purposes and all the differences arise from the single sign that differs.

A realistic theory must be able to deal with bosons as well as fermions. Moreover, it makes no sense to imagine that a theory should only treat bosons as fundamental particles or it should only treat fermions as fundamental particles. Why? 

If you have fermions, it is always possible to construct their bound states with an even number of fermions. These bound states inevitably behave as bosons and their properties are pretty much identical to the properties of elementary bosons: elementary and composite bosons (and other particles) should really be studied together, as we will argue. Moreover, real bosonic particles in an interacting theory (for example glueballs in QCD) also contain a mixture of fermionic particle-antiparticle pairs (for example quarks and antiquarks): one can never "remove all traces of fermions" from the real particles.

On the other hand, fermionic excitations can also emerge from a purely bosonic starting point but one needs more sophisticated methods than ordinary bound states, namely solitonic solutions and their excitations. However, a more important fact is that fermions are observed to exist and a remotely realistic theory simply has to agree with their existence.

To summarize, you should get used to the fact that a good enough theory has to contain both bosons and fermions, pretty much on equal footing, even though their physical manifestations in real-world, complex situations may look very different.

Particles of different spins in general

Bosons that like to be grouped with others can be shown to have an integer intrinsic angular momentum i.e. spin while the spin of fermions is half-integral such as 1/2 or 3/2. Particles, especially the nuclei, can have very high spins comparable to 10 or more.

However, the particles that you would ever consider "elementary" tend to have spins that never exceed 2. In fact, gravitons are the only elementary particles whose spin is 2: their polarizations with mixed signature (one time-like coordinate) would behave as "bad ghosts" that lead to negative probabilities. This potential catastrophe is prevented by gauge invariance, and the only possible gauge invariance for spin-2 fields is general covariance (diffeomorphism symmetry) of GR. 

In this setup, the tensor field (the metric tensor) has to couple to the conserved stress-energy tensor. There can only be one such tensor in a sensible interacting theory of one Universe, which is why there can only be one kind of a graviton. However, the graviton may be higher-dimensional and its Fourier decomposition into four-dimensional particles can lead to new types of particles (Kaluza-Klein modes of the graviton; graviphotons; new scalar fields).

Analogously, the removal of unphysical, ghostly modes of spin 3/2 particles requires a conserved spin-3/2 current, corresponding to a spin-1/2 conserved quantity. That's inevitably a "supercharge". Such a supercharge is inevitably fermionic, by the spin-statistics relationships, and the anticommutator of two copies of it inevitably includes translations. 

That's why we inevitably end up with diffeomorphisms as a part of the gauge invariance whenever there are spin-3/2 fields: we have a theory of general relativity with local supercharges, also known as supergravity, and the spin-3/2 fields are the gravitino fields. There can be a couple of them but not too many because the interactions become increasingly constrained as you add new supercharges.

The only elementary spin-1 fields are gauge fields such as the electromagnetic fields creating photons or their Yang-Mills counterpart connected with gluons or W bosons or Z bosons. The unphysical, ghostly, time-like component must be removed by a standard gauge invariance, Abelian or non-Abelian one. This gauge invariance can be unconfined and unbroken (like in electromagnetism), confined (like in the strong force) or spontaneously broken (like in the electroweak force) but it is still a gauge invariance, despite the very different behavior of these three types of gauge fields. The underlying mathematics is virtually identical in the three cases and all the qualitative differences in the everyday life are "emergent".

Spin-1/2 and spin-0 fields have no modes with negative probabilities. That's why they require no additional gauge invariances. These ordinary fields are often called "matter fields" (in the narrow sense) in particle physics. It is natural for the elementary spin-0 fields not to be easily observed because they can easily become very massive. On the other hand, the masses of spin-1/2 particles are often protected to be low.

As you can see, elementary fields can only have spin up to 2, and as you approach 2, they require an increasingly specific structure underlying them. That doesn't mean that particles with spins above 2 don't exist: the nuclei or highly excited closed strings surely do exist. But there's no way to write a sensible Lagrangian with a finite number of fields where they would be treated as elementary fields. Such a Lagrangian would need new, high-spin gauge symmetries to get rid of the negative probabilities (from the creation of timelike modes) and such complicated symmetries would require the interactions to essentially vanish for the corresponding Noether charges to be conserved.

Elementary vs composite particles

In the previous paragraphs, I discussed elementary particles as something very different from the composite ones. However, such a difference is only "qualitative" if one intends to describe physics by a particular classical Lagrangian (that can later be quantized). That means that certain fields are chosen to be fundamental - and the particles that they create are usually close to some real particles we can observe - while all interactions are added as small corrections.

In general, interactions are not that weak and the actual observed particles are not identical to the quanta of the fields in a Lagrangian. That also means you can't "qualitatively" distinguish which particles are fundamental and which particles are composite. In this sense, the difference is only useful for the people who write Lagrangians on a sheet of paper, not for people who only want to observe the reality.

If you go to the opposite extreme limit where the interactions become "infinitely strong", the question which fields are elementary and which fields are composites (or solitons, to be explained below) gets mixed up dramatically - in some sense, the answer is turned upside down. We will discuss this issue later.

Stable vs unstable particles

Some particles such as electrons and photons (and maybe even protons?) are stable, others such as the W boson decay after some time. Quite generally, particles are stable if there doesn't exist anything lighter with the same value of conserved charges that they can decay into. By the rules of quantum mechanics, the mass of unstable particles is complex, with the imaginary part being dictated by the width (essentially the inverse lifetime).

Stable particles have real masses, i.e. their width equals to zero.

You could think that this difference between stable and unstable particles is qualitative. But it is only as qualitative as the difference between 0 and another real number. Whether a particle is stable or not depends on dynamics, not on some predetermined categorization of the particles. If you learn the mathematics, it naturally treats stable and unstable particles in the same way - just the width is zero in the stable case. There's no "real" iron curtain between the two groups. More concretely, if a particle is unstable, it doesn't mean that it must be composite. 

The neutron is unstable and composite but it is not really "made out of" the decay products, i.e. of a proton, an electron, and an antineutrino (such a bound state would be more similar to a much larger Hydrogen atom). Instead, it is made out of three quarks (and some QCD mushed potatoes in it).

The W boson and the Higgs boson are also unstable but they are completely elementary fields of the Standard Model - a statement that is really uncontroversial in the case of the W boson and the controversy in the Higgs case is largely speculative in character. How can they decay if they are elementary? Well, they can. Particles in quantum field theory can be destroyed and created as long as the conservation laws are obeyed. If no law prevents a process from occurring, it will always occur with a nonzero probability or rate.

Real vs virtual particles, particles vs resonances

There is a related way to look at the same question. Unstable particles appear as resonances. For example, if you collide an electron and a positron, they can annihilate into "pure energy" and a Z boson may be born from this energy (because it doesn't carry any charges, anyway). If the total energy of the two initial particles is close to the Z boson mass, you will produce the Z boson quite often. But because the Z boson mass is complex - the Z boson has a nonzero width because it is unstable - you will produce it even if the total initial energy is slightly off. You will observe the Z boson as a resonance in the scattering of your electron and your positron.

The concept of a resonance is a method to see an unstable particle. It is really another aspect of the very same thing. Whenever you observe a resonance, you can never be certain that the resonance is connected with an elementary or a composite particle. It can be both: except for extremely weakly coupled theories (where all the interactions are weak), there is no God-given qualitative difference between elementary and composite particles.

Color neutral vs confined particles

Quantum Chromodynamics, QCD, offers us lots of new classes of particles. Generally, all particles that interact via the strong force and that can actually be observed in isolation (in reality) are called hadrons. The most important subclasses of hadrons are baryons (with 3 quarks plus mushed potatoes: e.g. protons and neutrons) and mesons (with a quark and an antiquark plus mushed potatoes: e.g. pions and kaons).

But there can exist other types of similar particles such as tetraquarks and pentaquarks (with four or five quarks, plus potatoes) or glueballs (with several gluons only, plus potatoes). These increasingly composite particles become increasingly less fundamental although one must often be careful about such statements because in a different description, with a different Lagrangian, they can be differently composite. For example, glueballs may be dual to some gravitons according to the AdS/CFT correspondence.

These hadrons are very different from the particles that are inserted as elementary fields to the QCD Lagrangian: gluons and quarks. We never observe gluons and quarks in isolation because they carry color and the color (strong charge) is so strongly interacting that it always forces all colorful particles to get neutralized and form color-neutral combinations. In reality, we only observe these elementary colorful particles as "jets": the elementary particle with color tries to escape but because of the strong interaction, other particles are being glued to it and as a result, you will create a stream of color-neutral particles going in the same direction as the original quark or gluon.

But at some deeper level, partons (quarks and gluons) are particles in the very same sense as hadrons. If you study particle physics at distances much shorter than the proton radius, the confinement won't influence you and you will see many colorful particles running inside a hadron. They will be described by the same kind of quantum fields that you can also effectively use at very long distances to describe hadrons. The description in terms of quarks and gluons will be more accurate and well-defined (the theory with these fields is renormalizable) but it will be further from the observational reality because it is the hadrons, and not the quarks and gluons, that we directly observe.

Elementary excitations vs solitons

I have explained that the difference between elementary and composite particles depends on a particular Lagrangian. In fact, more dramatic effects of this kind often occur. There exist particles that are more composite than the normal composite particles, the so-called solitons. Solitons may be identified with classical solutions of some classical field equations: the magnetic monopoles are among the most famous examples. They usually exist because they carry some topologically nontrivial subtlety, a topological charge, or a similarly qualitative feature.

When you quantize your field theory, you will find out that the classical solution behaves as an object that becomes just another species of a particle. It interferes with itself and it does all the things that you expect from other types of particles. If your original field theory was weakly coupled, the solitons usually end up being very heavy, with masses going like "1/g^2" where "g" is the coupling constant. Note that "g" goes to zero so "1/g^2" goes to infinity.

In string theory, there are several possible counterparts of the gauge coupling constant "g". It can be the closed-string coupling constant "g_{closed}" which is why string theory contains ordinary solitons (like NS5-branes and magnetic monopoles) whose mass goes like "1/g_{closed}^2". 

However, you may also identify "g", the gauge coupling from field theory, with "g_{open}", the interaction strength of the open strings that goes like "sqrt(g_{closed}). That's why string theory also contains a new, lighter kind of solitons, the D-branes, whose mass (or tension, if they have additional spatial dimensions) goes like "1/g_{open}^2 = 1/g_{closed}". If "g_{closed}" is small, this tension goes to infinity but it is smaller than "1/g_{closed}^2", the parametric dependence of the tension of the ordinary solitons such as NS5-branes.

However, when you send any of these "g" constants to infinity, these particles naturally become light. That's why you shouldn't be shocked that there often exists an equivalent, "S-dual" description of your theory where the role of "g" and "1/g" gets interchanged, much like the elementary particles and solitons. What used to be light small waves on some quantum fields become complicated extended solitons, and vice versa. This S-dual description in terms of the initially heavy objects is more likely to exist in supersymmetric theories where supersymmetry guarantees that the "1/g^2" or "1/g" formula for the mass (or tension) is correct even for large "g", and the object indeed becomes light when "g" is large.

Besides S-duality, modern quantum field theory and string theory offers other examples showing that whether or not a particle is elementary or whether it has an internal structure depends on the description - or the Lagrangian - you choose. Whenever possible, you should naturally choose a description in which all coupling constants are small (interactions are weak). However, such a choice doesn't exist in general. You must live with the fact that quantum field theories have to describe elementary and composite particles together which sometimes makes it very difficult to determine their properties. 

When you know your starting point, the elementary particles and their interactions, the problem may look straightforward. In general, such a choice either doesn't exist or it is not unique. There may exist quantum field theories that have no classical Lagrangians, i.e. no allowed choice of elementary fields, but they still predict everything about the particle species and forces that should exist in the world described by this theory. 

The (2,0) theory in 6 dimensions is believed to be an example. However, there may be a fivebrane minirevolution in the future that will show that this exotic theory actually has a universal Lagrangian, much like it recently happened with the 3-dimensional M2-brane theories.

Elementary particles vs black holes

The comments above should have convinced you that many (overlapping) types of particles belong to the "core" of the standard quantum field theory or they are linked by insights that have been well understood and "logically" follow from a purely theoretical analysis of quantum field theories: bosons, fermions, leptons, quarks, gauge bosons, gravitons, gravitinos, superpartners, atoms, molecules, animals, planets, stars, other complicated & composite bound states of known particles, solitons, hadrons, mesons, baryons, tetraquarks, pentaquarks, glueballs, neutrinos, Higgs bosons, magnetic monopoles, other solitons, wrapped D-branes, and many others. 

All of them may carry an energy/momentum vector, all of them may be associated with some fields, all of them interfere with themselves etc.

However, there exists an additional type of objects that seem different: black holes. Are they composed out of electrons or other known particles? It doesn't seem to be the case. In general relativity, black holes seem to be solitons, classical solutions of some classical field equations. However, quantum theory guarantees that black holes must come as well-defined species, the black hole microstates. They are macroscopically indistinguishable and their number is huge, comparable to "exp(S)", where "S" is the black hole entropy which is very huge because it is the event horizon area in Planck units, and the maximum entropy you can ever squeeze to the same volume.

Despite their very different origin, black hole microstates behave just like other types of particles. They will appear as resonances in a scattering. If you could isolate them in a situation where they are stable, they would interfere with themselves, and so on. Previously, we have seen that the number of possible particles can clearly be infinite because you can create many types of composite objects (such as stars) and they can be excited in very many ways.

But the black holes take this set of possibilities into the extreme because the number of black hole microstates exceeds any number we have previously discussed. They should have a well-defined spectrum with well-defined widths but because they are not really made out of electrons or other known elementary particles, it seems that we don't know any straightforward method to precisely calculate the spectrum of the black hole microstates. Nevertheless, string theory shows that the answer to this question is completely unique even if you can't say that the objects are made out of specific elementary building blocks. 

Quantum field theory vs string theory: what remains to be answered

String theory may be thought of as the most conservative extension of quantum field theory that adds gravity - with spin-2 gravitons - to the other forces and matter fields. It is a theory of quantum gravity and the black holes become the newest, most original type of particles that such an upgraded quantum field theory predicts.

On the other hand, string theory may also be viewed to be exactly as complicated an animal as a quantum field theory, due to the AdS/CFT correspondence. A string theory on a curved AdS-like space - which seems to be equally complicated as a quantum gravitational theory on a flat space - is exactly equivalent to a lower-dimensional non-gravitational quantum field theory on a flat space. So if you don't care about the spacetime dimensionality, gravitational and non-gravitational theories (QFTs or string theory vacua) seem to be equally complex.

Quantum field theory and string theory have been understood well enough for the people to qualitatively follow the nature of interference, interactions, scattering, poles in the interactions, confinement, spin, the role of gauge symmetries, and all other features of physics that were mentioned in the text above, besides other features that have not been mentioned.

However, these methods still don't exactly tell you what is the spectrum of particles and their masses. There are many options - there are many string-theoretical vacua and there are even more quantum field theories.  Despite the AdS/CFT-like equivalences, we usually want to talk about a differently filtered set of vacua when we talk about string theory vacua, and a differently filtered set of quantum field theories when we talk about quantum field theories. So the two sets are not really equally large.

In quantum field theory with a Lagrangian - that you can put on a lattice, among other approaches - you can completely calculate all physical phenomena, at least in principle. You will find out that if the theory is well-defined at very short distances, it must be completely specified by its qualitative spectrum at long distances and a few parameters (masses and coupling constants: the marginal and relevant deformations). So QFTs with a Lagrangian seem to form a set that is more or less understood.

QFTs without a Lagrangian are slightly more difficult. This class must include exotic theories such as the (2,0) theory in six dimensions. Nevertheless, it is natural to assume that this broader class, where the Lagrangian can be absent but where the other features of quantum field theory exactly hold, is comparably large to the class of QFTs with a Lagrangian.

In some sense, this class is similarly understood or misunderstood as the set of the string-theoretical vacua, also referred to as the landscape. It is important to note that even though we can't fully construct particles in a generic stringy vacuum out of a specific finite selection of elementary particles, the properties of all particles and interactions (including arbitrarily heavy black hole microstates) seems to be completely determined by the dynamics. For example, the black hole microstates in 11-dimensional M-theory can be calculated from the BFSS matrix model, at least in principle.

In some sense, this returns us to the framework of "bootstrap" - the idea that quantum field theories (and their extensions) are able to determine themselves, by obeying the basic consistency criteria, but without having any explicit methodology based on some preferred starting points (such as a set of elementary particles). This meme, originally promoted by Werner Heisenberg and heavily followed by the S-matrix theorists in the late 1960s, was largely unsuccessful (except for two-dimensional CFTs where it can be almost fully followed).

The history of physics has chosen a different path: all truly successful theories in the 20th century have always been constructed out of some specific starting points and elementary particles, such as quarks & gluons or relativistic strings. However, the recent duality revolution has shown that the choice of the elementary particles is not unique: in fact, there are many equivalent ways to approach a particular strongly-coupled quantum theory. In some sense, the number of classical Lagrangians is even higher than the number we need, i.e. than the number of physically distinct quantum theories.

On the other hand, the duality revolution also suggests that some theories or points on the landscape should exist even if we have no weakly-coupled description or a Lagrangian method based on elementary particles to approach the point. It is very tempting to ask what are the principles that can determine all properties of such theories without constructing them out of some specific elementary building blocks. However, we must realize that such a program is not guaranteed to be on the right path. It is a research project and its success may be a matter of a wishful thinking only.

While question marks remain, physics has already achieved an amazing degree of unification of its basic concepts that are enough to understand the observable world around us.

And that's the memo.

Not the Raptor Post I Was Expecting to Write [Science After Sunclipse]

Scienceblogs: Physical Science - 周二, 2009-01-06 01:19

Today's xkcd was insufficiently nerdy for me.

Yes, that's right.

In order to make the comic adequately reflect what I do on a daily basis, I have at least to modify the temperature conversion chart:

Read the rest of this post... | Read the comments on this post...

Coco the Colossal Colon

Impropable Research - 周二, 2009-01-06 01:02

“Coco,” as the Colossal Colon is affectionately known, is a 40-foot long, 4-foot tall oversized model of the human colon that is designed to educate about colorectal cancer and other diseases of the colon. Visitors who crawl through the Colossal Colon will see Crohn’s disease, diverticulosis, ulcerative colitis, hemorrhoids, cancerous and non-cancerous polyps, and various stages of colon cancer.

So says the Colon Club.

The Varieties of Crackpot Experience

Cosmic Variance - 周二, 2009-01-06 00:58

Frank Tipler is a crackpot. At one point in his life, he did very good technical work in general relativity; he was the first to prove theorems that closed timelike curves could not be constructed in local regions of spacetime without either violating the weak energy condition or creating a singularity. But alas, since then he has pretty much gone off the deep end, and more recently has become known for arguments for Christianity based on fundamental physics. If you closely at those arguments (h/t wolfgang), you find things like this:

If life is to guide the entire universe, it must be co-extensive with the entire universe. We can say that life must have become OMNIPRESENT in the universe by the end of time. But the very act of guiding the universe to eliminate event horizons - an infinite number of nudges - causes the entropy and hence the complexity of the universe to increase without limit. Therefore, if life is to continue guiding the universe - which it must, if the laws of physics are to remain consistent - then the knowledge of the universe possessed by life must also increase without limit, becoming both perfect and infinite at the final singularity. Life must become OMNISCIENT at the final singularity. The collapse of the universe will have provided available energy, which goes to infinity as the final singularity is approached, and this available energy will have become entirely under life’s control. The rate of use of this available energy - power - will diverge to infinity as the final singularity is approached. In other words, life at the final singularity will have become OMNIPOTENT. The final singularity is not in time but outside of time. On the boundary of space and time, as described in detail by Hawking and Ellis [6]. So we can say that the final singularity - the Omega Point - is TRANSCENDANT to space, time and matter.

All of the signs of classic crackpottery are present; the vague and misplaced appeal to technical terminology, the spelling mistakes and capital letters, the random use of “must” and “therefore” when no actual argument has been given. Two paragraphs later, we get:

Science is not restricted merely to describing only what happens inside the material universe, any more than science is restricted to describing events below the orbit of the Moon, as claimed by the opponents of Galileo. Like Galileo, I am convinced that the only scientific approach is to assume that the laws of terrestrial physics hold everywhere and without exception - unless and until an experiment shows that these laws have a limited range of application.

Compares self with Galileo! 40 points! There is really no indication that the person who wrote this was once writing perfectly sensible scientific papers.

Perhaps you will not be surprised to find that Tipler has now jumped into global-warming denialism. In just a few short paragraphs, we are treated to the following gems of insight (helpfully paraphrased):

People say that anthropogenic global warming is now firmly established, but that’s what they said about Ptolemaic astronomy! Therefore, I am like Copernicus.

A scientific theory is only truly scientific if it makes predictions “that the average person can check for himself.” (Not making this up.)

You know what causes global warming? Sunspots!

Sure, you can see data published that makes it look like the globe actually is warming. But that data is probably just fabricated. It snowed here last week!

If the government stopped funding science entirely, we wouldn’t have these problems.

You know who I remind myself of? Galileo.

Stillman Drake, the world’s leading Galileo scholar, demonstrates in his book “Galileo: A Very Short Introduction” (Oxford University Press, 2001) that it was not theologians, but rather his fellow physicists (then called “natural philosophers”), who manipulated the Inquisition into trying and convicting Galileo. The “out-of-the-mainsteam” Galileo had the gall to prove the consensus view, the Aristotlean theory, wrong by devising simple experiments that anyone could do. Galileo’s fellow scientists first tried to refute him by argument from authority. They failed. Then these “scientists” tried calling Galileo names, but this made no impression on the average person, who could see with his own eyes that Galileo was right. Finally, Galileo’s fellow “scientists” called in the Inquisition to silence him.

One could go on, but what’s the point? Well, perhaps there are two points worth making.

First, Frank Tipler is probably very “intelligent” by any of the standard measures of IQ and so forth. In science, we tend to valorize (to the point of fetishizing) a certain kind of ability to abstractly manipulate symbols and concepts — related to, although not exactly the same as, the cult of genius. (It’s not just being smart that is valorized, but a certain kind of smart.) The truth is, such an ability is great, but tends to be completely uncorrelated with other useful qualities like intellectual honesty and good judgment. People don’t become crackpots because they’re stupid; they become crackpots because they turn their smarts to crazy purposes.

Second, the superficially disconnected forms of crackpottery that lead on the one hand to proving Christianity using general relativity, and on the other to denying global warming, clearly emerge from a common source. The technique is to first decide what one wants to be true, and then come up with arguments that support it. This is a technique that can be used by anybody, for any purpose, and it’s why appeals to authority aren’t to be trusted, no matter how “intelligent” that authority seems to be.

Tipler isn’t completely crazy to want “average people” to be able to check claims for themselves. He’s mostly crazy, as by that standard we wouldn’t have much reason to believe in either general relativity or the Standard Model of particle physics, since the experimental tests relevant to those theories are pretty much out of reach for the average person. But the average person should be acquainted with the broad outlines of the scientific method and empirical reasoning, at least enough so that they try to separate crackpots from respectable scientists. Because nobody ever chooses to describe themselves as a crackpot. If you ask them, they’ll always explain that they are on the side of Galileo; and if you don’t agree, you’re no better than the Inquisition.

ShareThis

The Football Positioning System [Uncertain Principles]

Scienceblogs: Physical Science - 周一, 2009-01-05 23:47

It's NFL playoff time, which means that sports fans will be treated to the sight of the most high-stakes farce in sports, namely the ritual of "bringing out the chains" to determine whether a team has gained enough yards for a first down. We've all seen this: the play is whistled dead, a referee un-stacks the pile of players, picks up the ball, and puts it down more or less where the player was stopped. Then he tosses the ball into the middle of the field, to a second referee, who tries to replicate the spot closer to the center of the field. Then a guy on the sideline carrying a big stick (connected by a ten-yard chain to another stick held by another guy) tries to put the end of the stick at the same position as the ball.

Three plays later, the spotting procedure is repeated, and then the sticks are bought out to the center of the field, the chain is stretched taut, and they measure the position of the ball to the nearest millimeter. Because, of course, there's absolutely no error in placing the sticks.

The whole ritual is preposterous, and anybody with the slightest scientific inclination has to wonder: "Isn't there a better way of doing this?" So, what would be required to do a better job of this?

Read the rest of this post... | Read the comments on this post...

Roads and Radii [Built on Facts]

Scienceblogs: Physical Science - 周一, 2009-01-05 23:00

I was out of town (again) this past weekend, hence the posting shortage. Why in the world is it so much harder to find time to post during a nominal between-semester-break? I dunno, but it seems to be true. Free time doesn't scale the way you'd like.

One of the fundamental skill sets a physicist or really just about any scientist needs is to understand how quantities change scale. This is especially true when things change scale at different rates. I first noticed this particular instance of scaling phenomena while sitting in traffic in the city of Houston, Texas whose map (via Google) is printed below:

houston.png

Here at the same scale is the town where I spend most of my time: College Station, Texas.

collegestation.png

Not counting the very dense central regions of Houston, it's not to much of a stretch to say that a randomly selected patch of Houston's sprawl will look a lot like the interior of College Station in terms of population density. In any case the density is usually of the same order of magnitude. But the developed area of College Station is tiny compared to the developed area of Houston. So as an approximation pretend that both are of equal and uniform population density, and we'll try to use that fact to explain why traffic is so much worse driving through Houston than it is driving through College Station.

Such a simplification makes clear what the problem is. Pretend for simplicity that both Houston and College Station are circular. They aren't, but this additional simplification is a very gentle one which will only cause an error which is O(1). Now let's find a picture of a circle (this one from Wikipedia, with British spelling):

250px-CIRCLE_1.svg.png

Now imagine that the circle encloses each city. The Houston circle will clearly be much, much larger. The roads entering the city must cross through the perimeter of the circle. Only so many roads per unit perimeter can fit, just as only so many people per unit area can fit.

But the perimeter is proportional to the radius, and the area is proportional to the radius squared. That is, for cities of larger and larger radius the number of people within the city increases much faster than the number of roads that can support them. Triple the radius of the city and you can triple the maximum number of roads entering. But the number of people in the city will have increased by a factor of 3*3=9, leaving you behind.

Of course there's mitigating factors. College Station doesn't have nearly the number of incoming roads that its perimeter can support, nor does it have any need for commuter lanes, toll roads, or mass transit. All those things can greatly increase the efficiency of the roads supporting a city. But in the final analysis, eventually you'll have fought a losing battle and there will be some limit to the practical size of a city before traffic simply becomes unmanageable.

I imagine the traffic engineers reading this are unhappy with my very simplified model of the perimeter as the variable of interest, for obviously traffic and urban design are vastly more complicated. And that's perfectly true. The mathematics is however entirely implacable and makes the accomplishments of traffic engineers that much more impressive.

Read the comments on this post...

Incompleteness by Rebecca Goldstein [Uncertain Principles]

Scienceblogs: Physical Science - 周一, 2009-01-05 21:51

Rebecca Goldstein's Incompleteness: The Proof and Paradox of Kurt Gödel is another book in the Great Discoveries series of short books by noted authors about important moments in the history of science, and the people behind them. Previous volumes include Everything and More and A Force of Nature, both of which were excellent in their own way, and Incompleteness fits right in there with them.

As the subtitle makes clear, this is a book about Kurt Gödel's famous Incompleteness Theorem, which shows that any formal logical system complex enough to describe arithmetic must allow the formation of statements that are true, but cannot be proved to be true within that system. If you've always wanted to know what all the fuss over Gödel, Escher, Bach was about, but can't make it through, this book would be an excellent alternative. Goldstein does an excellent job of explaining the meaning of the theorem, putting it in historical context, and sketching out the unique way Gödel did the proof.

Of course, like all the other books in the series, the book also reflects the author's tastes and professional inclination. Goldstein is a philosopher, and so she uses the book to make an argument about Gödel's philosophy: that contrary to the common impression of the theorem as the work of some sort of mathematical postmodernist, Gödel was in fact a passionate and committed Platonist, firmly believing in the independent reality of mathematical ideas. To him, the important part of the theorem was that the unprovable statements were true, suggesting a wider and deeper mathematical universe than the formalist program would admit. He wasn't out to destroy mathematical truth, but to confirm and in some sense ennoble it.

I'm not qualified to evaluate the accuracy of this claim, but Goldstein makes a convincing argument. She also does an excellent job of putting the theorem in historical context, sketching out both the philosophical circles of Vienna where Gödel cut his teeth, and the formalist program of David Hilbert (among others) that his famous result overthrew. And, of course, no biography of Gödel could hope to avoid his personal eccentricities, and the tragic descent into paranoia that led to his death.

This is a very well-done book, and if you have any interest in mathematics or the history and philosophy thereof, I recommend checking it out.

Read the comments on this post...

Biweekly links for 01/05/2009

Michael Nielsen - 周一, 2009-01-05 18:53

Click here for all of my del.icio.us bookmarks.

ShareThis

Puzzling Solutions

Impropable Research - 周一, 2009-01-05 13:02

(That’s an excerpt from the article “Puzzling Solutions,” published in AIR 14:3.)

Changing Emotions

Overcoming Bias - 周一, 2009-01-05 08:05

Previously in series:  Growing Up is Hard

    Lest anyone reading this journal of a primitive man should think we spend our time mired in abstractions, let me also say that I am discovering the richness available to those who are willing to alter their major characteristics.  The variety of emotions available to a reconfigured human mind, thinking thoughts impossible to its ancestors...
    The emotion of -*-, describable only as something between sexual love and the joy of intellection - making love to a thought?  Or &&, the true reverse of pain, not "pleasure" but a "warning" of healing, growth and change. Or (^+^), the most complex emotion yet discovered, felt by those who consciously endure the change between mind configurations, and experience the broad spectrum of possibilities inherent in thinking and being.

        -- Greg Bear, Eon

So... I'm basically on board with that sort of thing as a fine and desirable future.  But I think that the difficulty and danger of fiddling with emotions is oft-underestimated.  Not necessarily underestimated by Greg Bear, per se; the above journal entry is from a character who was receiving superintelligent help.

But I still remember one time on the Extropians mailing list when someone talked about creating a female yet "otherwise identical" copy of himself.  Something about that just fell on my camel's back as the last straw.  I'm sorry, but there are some things that are much more complicated to actually do than to rattle off as short English sentences, and becoming a member of the opposite sex has to rank very high on that list.  Even if you're omnipotent so far as raw ability goes, it's not like people have a binary attribute reading "M" or "F" that can be flipped as a primitive action.

Changing sex makes a good, vivid example of the sort of difficulties you might run into when messing with emotional architecture, so I'll use it as my archetype:

Let's suppose that we're talking about an M2F transformation.  (F2M should be a straightforward transform of this discussion; I do want to be specific rather than talking in vague generalities, but I don't want to parallelize every sentence.)  (Oddly enough, every time I can recall hearing someone say "I want to know what it's like to be the opposite sex", the speaker has been male.  I don't know if that's a genuine gender difference in wishes, or just a selection effect in which spoken wishes reach my ears.)

Want to spend a week wearing a female body?  Even at this very shallow level, we're dealing with drastic remappings of at least some segments of the sensorimotor cortex and cerebellum - the somatic map, the motor map, the motor reflexes, and the motor skills.  As a male, you know how to operate a male body, but not a female one.  If you're a master martial artist as a male, you won't be a master martial artist as a female (or vice versa, of course) unless you either spend another year practicing, or some AI subtly tweaks your skills to be what they would have been in a female body - think of how odd that experience would be.

Already we're talking about some pretty significant neurological changes.  Strong enough to disrupt personal identity, if taken in one shot?  That's a difficult question to answer, especially since I don't know what experiment to perform to test any hypotheses.  On one hand, billions of neurons in my visual cortex undergo massive changes of activation every time my eyes squeeze shut when I sneeze - the raw number of flipped bits is not the key thing in personal identity.  But we are already talking about serious changes of information, on the order of going to sleep, dreaming, forgetting your dreams, and waking up the next morning as though it were the next moment.  Not informationally trivial transforms like uploading.

What about sex?  (Somehow it's always about sex, at least when it's men asking the question.)  Remapping the connections from the remapped somatic areas to the pleasure center will... give you a vagina-shaped penis, more or less.  That doesn't make you a woman.  You'd still be attracted to girls, and no, that would not make you a lesbian; it would make you a normal, masculine man wearing a female body like a suit of clothing.

What would it take for a man to actually become the female version of themselves?

Well... what does that sentence even mean?  I am reminded of someone who replied to the statement "Obama would not have become President if he hadn't been black" by saying "If Obama hadn't been black, he wouldn't have been Obama" i.e. "There is no non-black Obama who could fail to become President".  (You know you're in trouble when non-actual possible worlds start having political implications.)

The person you would have been if you'd been born with an X chromosome in place of your Y chromosome (or vice versa) isn't you.  If you had a twin female sister, the two of you would not be the same person.  There are genes on your Y chromosome that tweaked your brain to some extent, helping to construct your personal identity - alleles with no analogue on the X chromosome.  There is no version of you, even genetically, who is the opposite sex.

And if we halt your body, swap out your Y chromosome for your father's X chromosome, and restart your body... well.  That doesn't sound too safe, does it?  Your neurons are already wired in a male pattern, just as your body already developed in a male pattern.  I don't know what happens to your testicles, and I don't know what happens to your brain, either.  Maybe your circuits would slowly start to rewire themselves under the influence of the new genetic instructions.  At best you'd end up as a half-baked cross between male brain and female brain.  At worst you'd go into a permanent epileptic fit and die - we're dealing with circumstances way outside the evolutionary context under which the brain was optimized for robustness.  Either way, your brain would not look like your twin sister's brain that had developed as female from the beginning.

So to actually become female...

We're talking about a massive transformation here, billions of neurons and trillions of synapses rearranged.  Not just form, but content - just like a male judo expert would need skills repatterned to become a female judo expert, so too, you know how to operate a male brain but not a female brain.  You are the equivalent of a judo expert at one, but not the other.  You have cognitive reflexes, and consciously learned cognitive skills as well.

If I fell asleep and woke up as a true woman - not in body, but in brain - I don't think I'd call her "me".  The change is too sharp, if it happens all at once.

Transform the brain gradually?  Hm... now we have to design the intermediate stages, and make sure the intermediate stages make self-consistent sense.  Evolution built and optimized a self-consistent male brain and a self-consistent female brain; it didn't design the parts to be stable during an intermediate transition between the two.  Maybe you've got to redesign other parts of the brain just to keep working through the transition.

What happens when, as a woman, you think back to your memory of looking at Angelina Jolie photos as a man?  How do you empathize with your past self of the opposite sex?  Do you flee in horror from the person you were?  Are all your life's memories distant and alien things?  How can you remember, when your memory is a recorded activation pattern for neural circuits that no longer exist in their old forms?  Do we rewrite all your memories, too?

Well... maybe we could retain your old male brainware through the transformation, and set up a dual system of male and female circuits... such that you are currently female, but retain the ability to recall and empathize with your past memories as if they were running on the same male brainware that originally laid them down...

Sounds complicated, doesn't it?  It seems that to transform a male brain into someone who can be a real female, we can't just rewrite you as a female brain.  That just kills you and replaces you with someone re-imagined as a different person.  Instead we have to rewrite you as a more complex brain with a novel, non-ancestral architecture that can cross-operate in realtime between male and female modes, so that a female can process male memories with a remembered context that includes the male brainware that laid them down.

To make you female, and yet still you, we have to step outside the human design space in order to preserve continuity with your male self.

And when your little adventure is over and you go back to being a man - if you still want to, because even if your past self wanted to go back afterward, why should that desire be binding on your present self? - then we've got to keep the dual architecture so you don't throw up every time you remember what you did on your vacation.

Assuming you did have sex as a woman, rather than fending off all comers because because they didn't look like they were interested in a long-term relationship.

But then, you probably would experiment.  You'll never have been a little girl, and you won't remember going through high school where any girl who slept with a boy was called a slut by the other girls.  You'll remember a very atypical past for a woman - but there's no way to fix that while keeping you the same person.

And all that was just what it takes to ranma around within human-space, from the male pole to the female pole and back again.

What if you wanted to move outside the human space entirely?

In one sense, a sex change is admittedly close to a worst-case scenario: a fixed target not optimized for an easy transition from your present location; involving, not just new brain areas, but massive coordinated changes to brain areas already in place.

It might be a lot easier to just add one more emotion to those already there.  Maybe.

In another sense, though, a sex change is close to a best-case scenario: the prototype of your destination is already extensively tested as a coherent mind, and known to function well within a human society that already has a place for it (including companions to talk to).

It might be a lot harder to enter uncharted territory.  Maybe.

I'm not saying - of course - that it could never, ever be done.  But it's another instance of the great chicken-and-egg dilemma that is the whole story of present-day humanity, the great challenge that intelligent life faces in its flowering: growing up is a grownup-level problem.  You could try to build a cleanly-designed artificial grownup (self-improving Friendly AI) to foresee the pathway ahead and chart out a nonfatal course.  Or you could plunge ahead yourself, and hope that you grew faster than your problems did.

It's the same core challenge either way: growing up is an adult problem.  There are difficult ways out of this trap, but no easy ones; extra-ordinary solutions, but no ordinary ones.  People ask me why I take all these difficulties upon myself.  It's because all the easier ways, once you examine them in enough fine detail, turn out to be illusions, or contain just as much difficulty themselves - the same sort of hidden difficulty as "I'd like to try being the opposite sex for a week".

It seems to me that there is just an irreducible residue of very hard problems associated with an adult version of humankind ever coming into being.

And emotions would be among the most dangerous targets of meddling.  Make the wrong shift, and you won't want to change back.

We can't keep these exact human emotions forever.  Anyone want to still be eating chocolate-chip cookies when the last sun grows cold?  I didn't think so.

But if we replace our emotions with random die-rolls, then we'll end up wanting to do what is prime, instead of what's right.

Some emotional changes can be desirable, but random replacement seems likely to be undesirable on average.  So there must be criteria that distinguish good emotional changes from bad emotional changes.  What are they?

Czech EU presidency: Israel is defending itself

Luboš Motl’s Reference Frame - 周一, 2009-01-05 07:55



Israel defense force...

On Saturday, Mr Jiří František Potužník (George Francis Paw-tooh-zh-nick), the spokesman for the Czech prime minister, Mr Mirek Topolánek, the current boss of the rotating EU presidency, said an obvious fact about the current situation in the Middle East (see e.g. Deutsche Welle):
At the moment from our perspective we do understand that the action is part of the defensive action of Israel (...) we do understand that it is more defensive than offensive.
The Middle East issues became the first example of the theatrical character of the EU presidency. Of course that a smaller country can't change too many things in the EU even if it is a temporary president of the union and even if its opinions coincide with the official opinions of the world's only superpower.

The Czech politicians have clearly come under fire from the self-proclaimed exclusively politically correct European politicians who effectively sleep with the terrorists in Hamas. So it took a day and Mr Potužník was forced to apologize (AFP, Google News). Now, let me ask you: do you really think that Mr Potužník or Mr Topolánek have changed their opinion about this fundamental, basic question in 24 hours?

It's ludicrous, of course. What happened has clearly been a wave of intimidation and blackmailing from Paris, London, Berlin, and other cities. (Yes, the U.K. is against the right of Israel to defend itself.) Whether or not you agree with the Israeli strikes, the stories surrounding the Czech EU presidency show that democracy and freedom of thought in Europe is limited.

Is Mr Topolánek's opinion shared by all European politicians or citizens? It's surely not. But does the whole Europe denounce Israel? The answer is obviously No, too, even though some people would love to obscure this point.

Israel and Czechoslovakia: some history

Czechoslovakia was one of the main territories whose Jewish population was almost completely exterminated during the Nazi era. A fellow (former) Fellow in the Society of Fellows once visited me in Pilsen and took me into a place where I had never been before - a museum of holocaust (plus our synagogue, the third largest one in the world). I was shocked. 

Pilsen has contributed about 2,600 Jewish victims of the holocaust: virtually all of them had to die. The escalation of the anti-Jewish sentiments and policies (the disappearing Jewish right to own ski or talk to non-Jews etc.) during the 1930s was scary to follow because you can realize how easy it is for things to gradually drift in a very bad direction and how people today - or any other period of the history - have everything (bad) they need to evolve into the animals they became in the 1930s.



The Great Synagogue in Pilsen...

Clearly, the holocaust experience has strengthened the plans to recreate a Jewish state in Palestine in the late 1940s. It was a difficult and controversial engineering project meant to restore the status that existed 2,500 years ago or so - driven by the desire to transform the Jews into a generic nation with its own homeland, like everyone else - but I would claim that it has worked beautifully. 

Today, Israel is a prosperous, cultural, and democratic island inside the ocean of the 1st millenium religious bigotry and totalitarianism. Its mostly cultivated citizens are not responsible for any wrongdoings that took place in the late 1940s and their human rights and security deserve to be protected as much as those of German or French citizens. Of course, some hypothetical rights only matter if they can be enforced by someone - in this case by Israel's own power.

The existence of Israel used to be controversial but it should no longer be controversial today. The people who lived when the country was created are mostly dead today. The country has the same right to protect its integrity as any other civilized country in the broader Euro-Atlantic civilization space.

In the late 1940s, Czechoslovakia was naturally friendly towards Israel and it helped the country to overcome some of its first problems: that included arms shipments between 1947 and 1949. Regardless of the "capitalist" character of Israel, these policies were compatible with communism because our support for Israel was partly viewed as a part of our anti-Nazi attitudes.

It took quite some time - several decades - before the Czechoslovak communists began to treat Arafat and other terrorists as their "comrades". But this relationship was never too cordial, anyway. And Czechoslovakia has never become an enemy of Israel, after all. Clearly, after the collapse of communism, Czech and Slovak politicians did their best to fully restore our friendly relations with Israel and undo the relatively small harm caused by the previous support of the Arab socialist politicians.

Now, every Czech politician wants peace in the region - or at least everyone will tell you so. Most ordinary people don't care but whoever cares prefers human decisions. On the other hand, most people in the Czech Republic understand the actual dynamics of similar conflicts in the real world. If a country is not allowed to protect itself against an obvious enemy and/or if the allies leave it in its trouble, the country can cease to exist. It's as simple as that and we have quite some experience with this assertion.

So you know, a few Arab civilians who are killed on the broader Israeli territory are sad news. On the other hand, this sorrow is a sentiment that shouldn't obscure the long-term strategic thinking about the whole situation. If we began to be ambiguous about our support of Israel because we didn't like a particular strike, we could also see our ally to be inevitably defeated and replaced by a much less user-friendly system in a near future. And we could be very sorry about that.

Once again, let me repeat that I find it disgraceful for the French, German, British, and maybe even Italian officials to intimidate the Czech politicians who are now officially in charge of the EU, according to its own rules. These fags have the right to have sex with the officials in Hamas ;-) but they have no right to prevent the citizens of the EU to say something else about important questions such as the Palestine question than what they actually think, especially not during the Czech EU presidency. 

Most of us - including Mr Karel Schwarzenberg, the uniformly diplomatic aristocrat who is the Czech minister of foreign affairs - happen to agree with the U.S. politicians and not the French ones about this issue even though most of us want to avoid useless controversies, too. And unless the French and German officials want to reject the basic features of the European democratic space and merge the EU with the world of Islam, they should stop intimidating the Czechs and others. Instead, you should consider listening to and following your current leaders, the Czech Republic. 

Using all the languages of the Munich Treaty signatories: Merci, danke sehr, thank you, grazie. And that's the memo. ;-)

P.S.: Predictions for the future

While the Czech Republic will clearly be unable to promote the pro-Israel standpoint into an official EU policy, I am confident that the newly discovered diversity of the European opinions will be enough to give Israel a sufficient freedom to nearly solve these problems on its greater territory. Europe has been recently hurting Israel's potential to improve the situation, after all. Sometimes it's enough not to hurt someone.

You know, the situation over there is tough but it is not unsolvable, and a proper solution almost clearly requires a few splinters of wood to be cut. Israel has a sufficient technological and moral edge to suppress the problems on these territories and achieve what has been impossible since Clinton's and Bush's years, despite their politically correct attitudes that could never lead anywhere.

The Arab civilians say that they're afraid of their life, and so on. I will tell you something: that's what they should be doing, after all. Too many of them are a part of the problem. Many of them harbor the zealous terrorists whose existence is incompatible with a long-lived peace on the Israeli and Palestinian territory. The bulk of the most aggressive terrorists have to be killed, together with a couple of the civilians, to change their understanding what is possible or safe and what is not. Supporting Hamas militants can't be possible in a peaceful future and they must start to learn. Whether you like it or not, force is necessary for this lesson to be taught.

The confusing situation of the flipping U.S. presidents will surely give Israel an additional room to act. I am confident that they should kind of win after a few weeks and a full-fledged aggression of other Arab or Persian countries against Israel would eventually restore the status of the U.S. as an ally of Israel, so this counter-attack won't materialize.

Good luck to Israel and all of its Jewish, Arab, and other citizens who want the situation to converge into a stable, capitalist, democratic, not-religiously controlled state on the territory, naturally dominated by the Jewish nation. But the Czech Republic is going to help you by following the good soldier Švejk's example only. 



Click the picture of the French, EU, Czech foreign ministers to see a similar optimistic scenario by an Israeli professor.

I am personally convinced that the relative contribution of the Jewish nation to the modern civilization, including theoretical physics, vastly exceeds the ratio of the Israel's territory and the total land mass on Earth which is why I find it natural for Israel to be restored and stabilized within the borders of the Greater Israel we knew for a few decades.

And Things for Them to Blog About

Cosmic Variance - 周一, 2009-01-05 07:55

As the year breaks, the internets are abuzz with deep thoughts!

What will change everything? is this year’s Edge Annual Question. Many interesting answers, as you might expect. Choose from Massive Technological Failure (David Bodanis), Breaking the Species Barrier (Richard Dawkins), Coordinated and Expanded Computational Power (Lisa Randall), Faster Evolution (Jonathan Haidt), Happiness (Betsy Devine), Synthetic Biology (Dimitar Sasselov), and more. The book of last year’s question is out soon.

The blog posts to be reprinted in the Open Lab 2008 anthology have been announced — only 50 selections from over 500 nominations, I’m glad I wasn’t responsible for making the tough choices. Also glad that they chose one of my posts, The First Quantum Cosmologist. You can also read about The Igneous Petrology of Ice Cream (Green Gabbro), Expect the Unexpected (A canna’ change the laws of physics), How do cave bats know when it is dark outside? (Pondering Pikaia), and perhaps the most courageous blog post of all time: Liveblogging the Vasectomy (Terra Sigillata). Some sort of new journalism” going on there.

Finally, if all those ideas are weighing you down, play with the David Lee Roth ‘Runnin’ With the Devil’ Soundboard (via Cynical-C). Deconstructed from this classic track.

The complete version is here, but it only detracts.

ShareThis

Blogs That Should Exist

Cosmic Variance - 周一, 2009-01-05 02:48

I’m hoping that, for many of our readers, New Year’s Resolutions include getting off their duffs and starting a blog of their own. It’s certainly not hard; at the minimal level of effort, hop over to Blogger and set up your own free blog in a couple of easy steps. Only after you’ve established yourself can you hope to sell out to the Man and thereby cause the Death of the Blogosphere, like us.

But there are obstacles, for example: what to call the blog? We’re here to help. I was leafing through some old emails, and stumbled across the conversations we were having in the days before Cosmic Variance even existed. The heady days of youth, when we were trying to come up with good names for our new venture. Of course there are many types of blogs, from individual rants about the state of one’s personal life and recent dining experiences to focused discussions of the prospects for health care reform at the national level. We (including Clifford) wanted something that reflected our identity as scientists, but would attract and intrigue non-scientists as well, as we have always hoped to cast our discoursive net more widely than our particular disciplines. So we were looking for titles that played off scientific concepts, but didn’t come off as complete gobbeldy-gook to non-experts. Shores of the Dirac Sea is an excellent recent example of the genre — very much a physics in-joke, but one that isn’t completely off-putting to outsiders. If you call your blog “Laplace-Beltrami Operator” or “Gravitino Propagator,” you might amuse yourself, but your audience will be limited. (Apologies if there are any blogs out there with those names.)

Of course we came up with more than one, before settling on our perfect choice. But what was imperfect for us might fit you just fine. So, offered up free of charge, here are some of the names we were bandying around, plus some extras I came up with since.

  • Tycho’s Nose
  • Higher Dimensional Operators
  • Extremize The Action
  • Critical Phenomena
  • The Residue Theorem
  • But No Simpler
  • De Revolutionibus
  • Smooth Tension
  • Ultra Deep Field
  • Outside the Light Cone
  • Primeval Atom
  • Left As An Exercise
  • The Error Bar

Personally I’m partial to Tycho’s Nose, but The Error Bar is an awesome name. That blog practically writes itself. So what are you waiting for?

Those who are too lazy and/or timid to start their own blogs are encouraged to suggest additional names in comments.

ShareThis

Mars Rovers Still Working After Five Years [Aardvarchaeology]

Scienceblogs: Physical Science - 周日, 2009-01-04 21:20

Dear Reader, remember the remote-controlled Mars rovers, Spirit and Opportunity? How long is it since the last time you thought of them? Spirit landed on Mars five Earth years ago today, Opportunity on 25 January -- and both are still going strong! These machines were originally meant to work for three months, yet they continue to trundle around that cold, distant planet, taking pictures and analysing rocks. Check out the project's web site for news!

[More blog entries about , , , ; , , , .]

Read the comments on this post...

<em>n</em>Lab -- General Discussion

The n-Category Café - 周日, 2009-01-04 20:53
A place for general discussion concerning the nLab. urs http://www.math.uni-hamburg.de/home/schreiber urs.schreiber@math.uni-hamburg.de

Math in Washington D.C. [EvolutionBlog]

Scienceblogs: Physical Science - 周日, 2009-01-04 18:30

I will be leaving town tomorrow to spend most of this coming week in Washington D.C., participating in the annual extravaganza known as the Joint Mathematics Meetings. This is quite simply the place to be if you have any interest in mathematics.

Of course, this means I will only have limited internet access for the next few days. So I will not be blogging, and I will not be making detailed replies to comments. Try to soldier on in my absence!

Read the comments on this post...

Man *can* live by theory alone

Impropable Research - 周日, 2009-01-04 13:02

Can humans live completely according to a theory? Apparently so, if one uses the logic in Peter Huber’s book Hard Green: Saving The Environment From The Environmentalists A Conservative Manifesto. Huber writes:

Cut down the last redwood for chopsticks, harpoon the last blue whale for sushi, and the additional mouths fed will nourish additional human brains, which will soon invent ways to replace blubber with Olestra and pine with plastic. Humanity can survive just fine in a planet- covering crypt of concrete and computers.

聚合内容