Physics is a science and the experiment is the ultimate judge of the validity of the physical theories. At the same moment, the idea that the search for the truth in physics is just a sequence of mechanical tests of theories against well-defined experimental data that reveal the truth step by step is a narrow-minded illusion.

The ideas in physics are often much more far-reaching. Their importance often exceeds the impact of philosophical or religious dogmas. In fact, some ideas in physics are so far-reaching that they determine not only the answers but the character of the very questions that are going to be asked for many decades or centuries after the original ideas or principles are revealed. Sometimes we talk about "beauty" in physics but different people often have different features of the theories in mind.

I would prefer to be slightly more specific - as specific as a philosophical essay allows one to be. Some of the main values that may determine the depth of principles and theories in physics may be described as follows:

- uniqueness & rigidity
- inevitability
- self-consistency and mutual causal relations between different statements
- ability to avoid inconsistencies, especially if consistency is not guaranteed from the beginning; equivalently: the existence of miraculous cancellations of inconsistencies
- limited number of independent assumptions
- ability to be relevant in a large number of situations
- power to organize previous systems of ideas and reveal new relations between them
- multiplicity of descriptions of the same structure that are mathematically equivalent
- the maximal possible yet finite amount of complexity of these theories that still makes them compatible with fundamental principles

While I find it obvious that all of these features are important and contribute to the feeling that an idea or a whole framework is on the right track, each of these characteristics has its foes. In fact, there are many people who will tell you that each of these properties is in fact a disadvantage.

Many people will tell you that their proposed theory is good because it is not unique. They will try to convince you that their theory is good exactly because one can deform it in a huge number of ways. One can add anything to these theories. Well, I beg to differ. Valuable theories are always very special animals. Given some assumptions or principles - that must themselves be deep and we will mention some examples later in the text - a valuable theory must be unique or nearly unique. It must look like a golden needle in a haystack. And the criteria that determine which particle is a golden needle must be universal and robust, too.

The mathematical ideas of calculus invented by Newton and Leibniz were inevitable and in some sense unique. The actions defining laws of classical mechanics are not too numerous. The rules of field theory become even more constrained once we assume a beautiful principle such as the Lorentz symmetry. The principles of quantum mechanics are the unique extension of the naive classical deterministic laws that is compatible with the basic rules of logic. The Lagrangians for renormalizable field theories are extremely special because generic Lagrangians lead to a breakdown of the theories at higher energies.

Yang-Mills interactions are inevitable because they are the only known way how the interactions may grow weaker at shorter distances. Their structure requires us to consider theories with local gauge symmetries which are themselves "beautiful" and constrain the matter spectrum and the character of the interactions.

Let me now assume that the reader understands that the theories must be very special and predict a maximal number of consequences from a minimal number of independent assumptions. We don't necessarily need to minimize the number of assumptions and independent concepts as much as we can. Instead, we may work with a larger number of assumptions and objects, but we must always appreciate when some of the assumptions imply others - so that the set of assumptions does not feel disconnected.

**It is not "bad circular reasoning" but rather "good rigidity"**

Much like all other positive values in physics, connectedness of the ideas has its enemies. Some people will argue that a theory is not good enough because it is based on circular reasoning. This is an argument that some philosophers are ready to use against intellectual structures that are as essential as the theory of relativity - a system of ideas that is more impressive than all ideas ever invented by all philosophers combined.

Is it bad that different statements in relativity follow from each other? Not at all. Every theory must have *some* assumptions. And if the assumptions tend to imply each other - while still being able to underlie non-trivial and numerous predictions that may even confirm the experiments - we should definitely be more happy, not less happy.

Quantum field theories have the feeling of "relative uniqueness" and string theory offers an "absolute uniqueness" - the first theory the humans ever knew that is capable to do so. This statement does not mean that string theory only has one solution. Of course, it can have many "classical" solutions, asymptotic conditions, and huge Hilbert spaces built upon them. But the dynamical laws that determine which of these spacetimes and states exist and how they evolve are completely unique.

Whenever I talk with someone outside the mainstream high-energy physics, it becomes very clear that many people at the suburbs of the field have absolutely no understanding for these basic principles.

**Simplicity and beauty**

Another notion that very many people seem to misunderstand is simplicity. Are the laws of Nature simple? Well, it depends how you define the word "simple". We may start with the definition that the laws of Nature are accessible to people with a minimum required IQ, education, or effort. Are the laws of physics simple in this sense? No way. Indeed, as our understanding of Nature deepens, one must - fortunately or unfortunately - learn ever more profound concepts that become increasingly inaccessible to ordinary people and sometimes even to the experts.

**Simplicity vs. brevity**

Let us try another definition of simplicity. Simplicity may also be defined as the number of T-shirts or pages that we need in order to print all essential rules that will be comprehensible to an intelligent reader. Is Nature simple in this sense? Well, this definition is closer to the truth than the previous one. Indeed, many defining formulae of physics are very short and efficient.

But some of them may be rather long - but equally or more beautiful or fundamental. For example, the full Lagrangian of 11-dimensional supergravity is a rather complicated monster but it does not make it any less beautiful. What is important is that the individual terms in the Lagrangian are not independent from each other. In fact, the whole structure of the two-derivative Lagrangian is uniquely determined by the requirement of supersymmetry.

One of the comments in the list above was a variation of Gell-Mann's totalitarian principle: everything that is not forbidden is compulsory. We should always consider the most general theory that respects the same symmetries and other principles and is equally consistent as the first idea in the class of theories that we have encountered, discovered, or invented. We should never focus on a special, randomly chosen theory that does not differ from many others by the validity of any fundamental principle. We should never try to fool ourselves and others by pretending that such a randomly chosen representative is more important than other random elements of the same set. And we should never study theories with infinitely many parameters, all of which are strongly relevant for the questions that the theory is supposed to answer.

While Gell-Mann would probably think about our duty to add all couplings that respect the rules of the game, it is true that we must also accept all discrete choices for our theories that respect the same principles. Some of these theories may look rather complicated - for example, some people may think that the "E8 x E8" group of a ten-dimensional heterotic string background is too large - but similar theories are important nevertheless because of much more crucial reasons that a naive notion of simplicity.

**Symmetries and other valuable principles**

When I said "supersymmetry", it is indeed a good opportunity to mention what are the important principles that distinguish which object is the golden needle in a haystack of ideas. Some of the previous "valuable ideas" could be added to this list if we interpret them slightly differently. But we must also include more concrete principles that seem to be absolutely true in the real world, according to everything we know:

- Basic postulates of quantum mechanics - observables are linear operators on a Hilbert space and time evolution is given by another linear operator
- The evolution operators must be unitary to preserve the total probability since the probabilities are computed from squared complex amplitudes
- Dynamics must be local, at least approximately; we discussed locality here; locality is related to causality, another important principle
- Important symmetries should be respected

Symmetries of course play an important role in the scheme of things. Which symmetries do we mean? First of all, it turned out that the discrete symmetries are not terribly constraining and Nature does not care about them too much. People used to think that there was no difference between the left hand and the right hand; between particles and antiparticles. People used to think that C, P, T, and CP were symmetries of Nature.

Today we know better. These symmetries are broken and only the CPT symmetry seems to be the ultimate rule that survived. And it is only true because it can be interpreted as a particular element of a properly extended continuous symmetry, namely the Lorentz symmetry.

**The Lorentz symmetry**

Well, the Lorentz symmetry and its affine extension, the Poincaré symmetry, is an extremely important principle. This symmetry is a fundamental pillar of special relativity and it includes, via Noether's theorem, the conservation of energy, momentum, angular momentum, and the uniform motion of the center of mass. This symmetry relates many physical phenomena that were considered to be independent: magnetism is an inevitable supplement of electricity once the Lorentz symmetry is assumed. The existence of conserved energy follows from the existence of conserved momentum and vice versa. Moreover, the mass and the energy have to be equivalent and convertible to each other. Many other effects and notions that were independent are unified.

**General relativity as a generalization of special relativity**

Some people are extremely confused about the nature of special relativity and they will tell you that the discovery of general relativity has revoked the constraints imposed by special relativity. But that's another extremely deep misunderstanding of physics. General relativity is called general relativity because it generalizes special relativity; it does not kill it. One of the fundamental pillars of general relativity is the equivalence principle that states that in locally inertial frames, the laws of special relativity must be satisfied by all local phenomena.

The global Poincaré symmetry of special relativity is extended - or generalized - to the local diffeomorphism symmetry of general relativity. All observers are equally good for formulating the laws, not only the inertial observers. For a simple topology of spacetime, the symmetry of special relativity is a very small subgroup of the symmetry group of general relativity. For other topologies such an embedding can be more subtle but it is important to see that the laws of physics are still constrained by equally strong rules like those in special relativity. The idea that the constraints of special relativity may be forgotten after the papers published in 1915 is a symptom of a breathtaking ignorance.

Some of these people will tell you that the Lorentz symmetry is broken by particular backgrounds or solutions in general relativity and therefore it is no longer important. Well, Lorentz symmetry is *spontaneously* broken by virtually all configurations you can imagine - both in general relativity as well as special relativity - but in both cases, it is a *spontaneous *symmetry breaking. What is important is that the underlying *laws* respect the symmetry: the diffeomorphism and the local Lorentz symmetry of physics. A correct theory based on general relativity must admit a Minkowski (or de Sitter or anti de Sitter, which are equally constraining) solution.

**Local vs. global symmetries**

The diffeomorphism group is a local symmetry and at the quantum level, all states must be invariant (singlets) under all these local symmetries, much like in the Yang-Mills case. This is why the representation theory of the local, infinite-dimensional gauge groups is irrelevant for physics. On the other hand, states do not have to be invariant under global symmetries such as the Lorentz symmetry, which is why the representation theory of the global symmetries is physically important.

Special relativity is embedded in general relativity in such a way that its global symmetries become generalized examples of diffeomorphisms - that are however "large" in the sense that they are not generated by normalizable modes and therefore are not required to keep the physical states invariant. The generators of time translations and similar geometric operations map the points in the asymptotic regions of the spacetime to other points, and this property is enough to revoke the requirement that the physical states must be invariant under such operations. This is why non-zero (ADM) energy and momentum is possible even in the context of general relativity, even at the quantum level.

Even though the details how the requirement of the Lorentz symmetry - and analogously unitarity - is realized in a given formalism may be subtle, it is absolutely essential to realize that these principles must still hold, and if they are replaced by something else, this "something else" must be at least equally constraining as the original symmetries were in the original theories. Sorry to say but those who say that one can simply forget about unitarity or the Lorentz symmetry altogether are simply idiots.

**Cheapness of field redefinitions**

Some people are impressed, for scientifically unjustifiable reasons, by random field redefinitions and random functions into which various observables are substituted. Imagine that you are an economist and you invent that instead of the interest rate "X", you should study "Gamma(-1/X)". Because you know the Gamma function, you will say that it is an extremely advanced idea in economics to use "Gamma(-1/x)" instead of "X".

Of course, this example is one of the most pathetic example of a meaningless mathematical masturbation that you can invent. Nevertheless, some people apparently like to play with useless and unjustifiable constructions that are not unsimilar to one from the previous paragraph. Note that if you just redefine some things, you don't gain new physics, new ideas, or new principles. What can happen is that it becomes easier to solve a certain problem and/or invent a new idea or a principle. But one can always translate the insights to the previous variables. At the end, one should be using the variables in which the important features of the physical system are most transparent.

If a system of equations looks "simple" in a random unnatural choice of variables - in which the important principles don't look transparent - then such a "simplicity" is a disadvantage, not an advantage.

Inventing a convoluted system of formulae just because someone likes to obscure things is not tolerable in physics. A random new choice of variables is only justified if it allows one to find some important, unique, universally relevant new solutions, or if it is helpful to illuminate the validity of some key principles - such as unitarity, finiteness, Lorentz symmetry, or some kind of duality. Changes of variables that can't do anything like that have no room in physics. One can never assume that a random change of variables will lead to an interesting new physical idea without having any evidence, and one should never believe the people who are building their perceived "depth" on obscuring things by introducing physically unjustifiable changes of variables.

**Dualities and multiplicities of equivalent descriptions**

Finally, I want to mention dualities as another feature of theories that are likely to be deep and on the right track. Dualities and multiple descriptions of the same physics certainly did not start with string theory.

Classical physics could have been described by the Lagrangians as well as Hamiltonians. One could have used different coordinates and trivially show that the laws were equivalent. More strikingly, quantum mechanics could have been formulated in the Schrödinger picture, the Heisenberg picture, the Dirac mixed picture, or in terms of the Feynman path integral. The wavefunctions could be represented by functions of coordinates, functions of momenta, or discrete columns of complex numbers that encode the amplitudes of various energy eigenstates. All these approaches turned out to be equivalent although it was not obvious from the beginning.

Is it a bad thing for a theory to have many equivalent languages or formalisms? No way. It was one of the extremely important hints that quantum mechanics was a deep structure. Today, the mathematical facts behind these equivalences look trivial to most of us. But we have new, more impressive equivalences in string theory whose validity seems obviously true but whose "proof as clear as skies" is not yet accessible. In the future, people will most likely find new insights that will make the dualities and equivalences between different descriptions of string/M-theory more transparent. But the very fact that there exists some equivalence that is not immediately obvious suggests that there is something really intriguing to study.

The previous sentence contains the word "immediately". Indeed, if the equivalence of two pictures is immediately obvious, we don't want to count the multiplicity of descriptions as an argument for anything or against anything. The fact that we can use different letters or metric conventions or other conventions (including field redefinitions discussed above) does not mean that we necessarily deal with a deep set of ideas. In fact, it is always possible to formulate any kinds of ideas in different languages. We can only conjecture that we are facing an important idea if the equivalence between the different descriptions that superficially looked inequivalent takes some time and reasoning to be revealed.

Much like in the cases of all other important values in physics, many people are so profoundly confused that they count multiplicity of equivalent - but not manifestly equivalent - descriptions as a disadvantage. On the contrary, these people often prefer narrow-minded formalisms that can only be formulated in one way. They like if their proposed theories can't be connected with other ideas. They like if their colleagues have only mastered one small segment of mathematics. They like if their theories can only be written in the Hamiltonian form but not the path integral form. They don't mind if different approaches that normally lead to the same results give contradictory results in their case.

I beg to differ. Theories should be connected with all formalisms we have used to describe all important classes of phenomena in the past. All methods we have learned in the past should have a correct and sharp generalization that allows us to treat the newly proposed theory. The existence of several non-equivalent approaches is always an advantage. It is a practical advantage when we try to solve or understand the theory: much like other symmetries, dualities can help us to solve particular problems. At the same moment, it is a hint that we are uncovering a huge empire in the world of ideas, not just a fiber in haystack.

We should always remember which features of the ideas and theories that we think about suggest that something important is being uncovered, and we should always point out if someone tries to replace deep and viable principles by shallow, random and unjustifiable dogmas.

And that's the memo.

## snail feedback (1) :

"General relativity as a generalization of special relativity

"Some people are extremely confused about the nature of special relativity and they will tell you that the discovery of general relativity has revoked the constraints imposed by special relativity. But that's another extremely deep misunderstanding of physics. General relativity is called general relativity because it generalizes special relativity; it does not kill it. One of the fundamental pillars of general relativity is the equivalence principle that states that in locally inertial frames, the laws of special relativity must be satisfied by all local phenomena."

I just don't believe you don't understand that general covariance in GR is the important principle, that accelerations are not relative and that all motions at least begin and end with acceleration/deceleration.

The radiation (gauge bosons) and virtual particles in the vacuum exert pressure on moving objects, compressing them in the direction of motion. As FitzGerald deduced in 1889, it is not a mathematical effect, but a physical one. Mass increase occurs because of the snowplow effect of Higgs boson (mass ahead of you) when you move quickly, since the Higgs bosons you are moving into can't instantly flow out of your path, so there is mass increase. If you were to approach c, the particles in the vacuum ahead of you would be unable to get out of your way, you'd be going so fast, so your mass would tend towards infinity. This is simply a physical effect, not a mathematical mystery. Time dilation occurs because time is measured by motion, and if as the Standard Model suggests, fundamental spinning particles are just trapped energy (mass being due to the external Higgs field), that energy is going at speed c, perhaps as a spinning loop or vibrating string. When you move that at near speed c, the internal vibration and/or spin speed will slow down, because c would be violated otherwise. Since electromagnetic radiation is a transverse wave, the internal motion at speed x is orthagonal to the direction of propagation at speed v, so x^2 + v^2 = c^2 by Pythagoras. Hence the dynamic measure of time (vibration or spin speed) for the particle is x/c = (1 - v^2/c^2)^1/2, which is the time-dilation formula.

As Eddington said, light speed is absolute but undetectable in the Michelson-Morley experiment owing to the fact the instrument contracts in the direction of motion, allowing the slower light beam to cross a smaller distance and thus catch up.

‘The Michelson-Morley experiment has thus failed to detect our motion through the aether, because the effect looked for – the delay of one of the light waves – is exactly compensated by an automatic contraction of the matter forming the apparatus…. The great stumbing-block for a philosophy which denies absolute space is the experimental detection of absolute rotation.’ – Professor A.S. Eddington (who confirmed Einstein’s general theory of relativity in 1919), Space Time and Gravitation: An Outline of the General Relativity Theory, Cambridge University Press, Cambridge, 1921, pp. 20, 152.

Einstein said the same:

‘Recapitulating, we may say that according to the general theory of relativity, space is endowed with physical qualities... According to the general theory of relativity space without ether is unthinkable.’ – Albert Einstein, Leyden University lecture on ‘Ether and Relativity’, 1920. (Einstein, A., Sidelights on Relativity, Dover, New York, 1952, pp. 15-23.)

Maxwell failed to grasp that radiation (gauge bosons) was the mechanism for electric force fields, but he did usefully suggest that:

‘The ... action of magnetism on polarised light [discovered by Faraday not Maxwell] leads ... to the conclusion that in a medium ... is something belonging to the mathematical class as an angular velocity ... This ... cannot be that of any portion of the medium of sensible dimensions rotating as a whole. We must therefore conceive the rotation to be that of very small portions of the medium, each rotating on its own axis [spin] ... The displacements of the medium, during the propagation of light, will produce a disturbance of the vortices ... We shall therefore assume that the variation of vortices caused by the displacement of the medium is subject to the same conditions which Helmholtz, in his great memoir on Vortex-motion, has shewn to regulate the variation of the vortices [spin] of a perfect fluid.’ - Maxwell’s 1873 Treatise on Electricity and Magnetism, Articles 822-3

Compare this to the spin foam vacuum, and the fluid GR model:

‘… the source of the gravitational field can be taken to be a perfect fluid…. A fluid is a continuum that ‘flows’... A perfect fluid is defined as one in which all antislipping forces are zero, and the only force between neighboring fluid elements is pressure.’ – Professor Bernard Schutz, General Relativity, Cambridge University Press, 1986, pp. 89-90.

Einstein admitted SR was tragic:

‘The special theory of relativity … does not extend to non-uniform motion … The laws of physics must be of such a nature that they apply to systems of reference in any kind of motion. Along this road we arrive at an extension of the postulate of relativity… The general laws of nature are to be expressed by equations which hold good for all systems of co-ordinates, that is, are co-variant with respect to any substitutions whatever (generally co-variant). …’ – Albert Einstein, ‘The Foundation of the General Theory of Relativity’, Annalen der Physik, v49, 1916.

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