25 Critical Comments

R. P. Feynman

 

The real problems in gravitational theory are: 

1To understand classical relativistic gravity without the complications of other things. 

2The general theory of cosmology because we may be able to work out the shape of the world. 

3To study the theory to see if anything new is in it which is not contained at first sight. 

4To learn from the philosophy of gravity something to use in other fields such as we have made use of the invariance principles and the ideas of Einstein. 

5Curiosity 

There exists, however, one serious difficulty, and that is the lack of experiments. Furthermore, we are not going to get any experiments, so we have to take a viewpoint of how to deal with problems where no experiments are available. There are two choices. The first choice is that of mathematical rigor. People who work in gravitational theory believe that the equations are more difficult than in any other field, and from my viewpoint this is false. If you then ask me to solve the equations I must say I can't solve them in the other fields either. However, one can do an enormous amount by various approximations which are non-rigorous and unproved mathematically, perhaps for the first few years. Historically, the rigorous analysis of whether what one says is true or not comes many years later after the discovery of what is true. And, the discovery of what is true is helped by experiments. The attempt at mathematical rigorous solutions without guiding experiments is exactly the reason the subject is difficult, not the equations. The second choice of action is to “play games” by intuition and drive on. Take the case of gravitational radiation. Most people think that it is likely that this radiation is emitted. So, suppose it is and calculate various things such as scattering by stars, etc., and continue until you reach an inconsistency. Then, go back and find out what is the difficulty. Make up your mind which way it is and calculate without rigor in an exploratory way. You have nothing to lose: there are no experiments. I think the best viewpoint is to pretend that there are experiments and calculate. In this field since we are not pushed by experiments we must be pulled by imagination. 

The questions raised in the last three days have to do with the relation of gravity to the rest of physics. We have gravity - electrodynamics - quantum theory - nuclear physics - strange particles. The problem of physics is to put them all together. The original problem after the discovery of gravity was to put gravity and electrodynamics together since that was essentially all that was known. Therefore, we had the unified field theories. After quantum theory one tries to quantize gravity. As far as the two methods of quantization are concerned, I believe that if one works the other will work. The crucial problem is to be able to tell when we have succeeded in quantizing the gravitational field. We should take the same attitude as in other branches of physics and compute the results of some experiments. We don't have the experiments and thus we do not know which results to calculate. However, if someone brought an experimental fact could we check it? Certainly, we can take a linearized approximation and the answer will be right or wrong. The reason for stressing experiments is because of quantum electrodynamics which was worked out in 1928 but was full of difficulties such as the infinite energy levels of the hydrogen atom. When Lamb discovered the spacing between two levels was finite, Bethe then got to work and calculated the difference and introduced the ideas of renormalization. We knew that the number was finite, but someone measured it and thus forced the computation. The real challenge is not to find an elegant formalism, but to solve a series of problems whose results could be checked. This is a different point of view. Don't be so rigorous or you will not succeed. 

Quantum mechanics and gravity do have something in common. The energy in quantum mechanics is best given by describing how the wave function changes if one solves the coordinate system a little bit, and gravity is connected with just such transformations of coordinates. Thus, the group-theoretic definition of energy and momentum in quantum theory is not very far away from the geometric connection between energy and what happens when you move the coordinate system. 

The connection of gravity with the other parts of physics (nuclear and strange particles) was not mentioned here. This is interesting and strange because from the point of view of a non-specialist there is just as much physics in these other fields. From the experimental side we have much more detail there but have no beautiful theory. 

Instead of trying to explain the rest of physics in terms of gravity I propose to reverse the problem by changing history. Suppose Einstein never existed, and his theory was not available, but the experimenters began to discover the existence of the force. Furthermore, suppose one knows all the other laws known now including special relativity. Then people will say we have something new, a force like a Coulomb force. Where did it come from? There will be two schools of thought. First, some people will say this force is due to a new field and second some people will say that it is due to some effect of an old field which we do not recognize. I have tried to do this forgetting about Einstein. 

First I will do the case of the new field. The force is proportional to and thus it must be mass zero field. Also, I assume that later one gets experiments about the precession of orbits so that the rate of motion does not appear to be proportional to the mass. Someone would try scalar fields, vector fields, ..., and so on. Sooner or later one would get to a spin two field and would say perhaps it is analogous to electrodynamics. Then he would write down 

or in place of the second term 

and in place of the fourth term 

In all this is the new field under investigation. 

From this one gets some second order equations roughly of the form 

Also the equation of motion of the particles is 

where is just a shorthand for . The field equations of electrodynamics have a property that the current conservation is an identity from the field equations. 

Now one asks what is equal to such that we get automatically ? Now, when one puts in the second power of the first derivatives of in the action he gets something definite. Incidentally, one gets the linearized form of the gravity equations. If now these equations are solved to see if any progress has been made, one deduces that light is deflected by the sun. One at this point might say that we know too much, that a field theorist would never have thought of this important conservation theorem. This is not true. Pauli deduced this equation without looking for gravity, but by asking himself what must the field equations be for fields of arbitrary spin. Soon someone would realize that something is wrong, for if particles move according to the equation of motion, which they must do from the given action, then the doesn't satisfy the correct equations. A suggestion, then, would be to add the field energy into the stress energy tensor and say that this also is a source of gravity. Then, would become . However, this would not work because a variation of the 's gives not only what one wants, but some new terms. Finally one asks if there exists an expression of third order in the 's which can be used in the action of the form and will give any relief from the difficulty. It is possible to prove from the definition of and the equation of motion that the true must satisfy some equation of the form 

Then one can go to the next higher order of approximation and this approximation will explain the perihelion of Mercury. Although one is on the right track this process is just an expansion. It is possible, however, to solve the problem mathematically by finding an expression which is invariant under 

To get the solution of this problem one asks a mathematician. However, it could have been solved by noticing that it is a geometric transformation in a Riemannian space. Finally, someone might suggest that geometry determines the metric. This would be a marvellous suggestion but it would be made at the end of the work and not at the beginning. 

What does one gain by looking at the problem in this manner? Obviously, one loses the beauty of geometry but this is not primary. What is primary is that one had a new field and tried his very best to get a spin-two field as consistent as possible. 

I think quantization would proceed in the same direction as the original solution of the problem. One would consider this just another field to be quantized. From the other viewpoint the geometry is important, but from this viewpoint gravity is just another field. I am sure that an enormous amount of formulae would be collected without having the generally covariant quantum theory. I advertise that this new point of view may, in fact, succeed in the end. Certainly people would not think that the rest of physics could be deduced from gravity. They may well be wrong, but it also may be true that gravity is just one more of a long list of difficult things that some day have to be put together. 

Now let us go to the second possibility, old fields. The physicists might try to explain the new force on the basis of the incomplete cancellation of electric charges of the order (number of particles) or some such scheme. However, there are a number of interesting possibilities which are not completely impossible. One important fact is that this field has an infinitesimal coupling constant and already one knows about one weakly coupled field, the neutrino. Also, the neutrino has zero rest mass which is needed for dependence. The neutrino equation is modified, for convenience, to read 

and the neutrino propagators are assumed to be . A first trial might be the single exchange of a neutrino between the two interacting bodies. In this case, however, a law does not result because the initial and final states are orthogonal. Another possibility is a two neutrino exchange, but this gives a potential which falls off faster than . Next, one could try one neutrino exchange between the two bodies with each body exchanging one neutrino with the rest of the universe. The rest of the universe is assumed to be at some fixed distance, . This does give rise to a potential which varies as . However, the amount of matter varies as so that upon integration over the universe one gets a logarithmic divergence. The most serious difficulty with this approach is, however, the large effect the sun would have on the earth-moon system. This last trial was so much better than the others one can go a step further and try a four neutrino process with the additional neutrino being exchanged in the rest of the universe. This will also give a potential and a higher order divergence and one must worry about the density of matter, etc. Higher order terms are possible but they are much more difficult to handle. Therefore, the possibility exists that the material from the outside is making the source of gravitation here through the exchange of well known particles, the neutrinos. This is obviously no serious theory and is not to be believed. For one thing the use of the correct propagators would change the dependence. If one did put in things correctly and got a finite amount for a result, then this is very curious and has not been noticed before. That is one of the advantages of looking at something from a different direction. Anyway, this is what the people who believe in old theories would do. 

This different point of view has been advertised in the hope that a few people will start looking at gravitation from a different direction. I think really that it is more likely and more interesting to go from the geometric side, but if a few investigations change directions we may get somewhere. 

ROSENFELD comments that the possible connection between neutrinos and gravitation was discussed a long time ago. Also, one says that gravitational energy is carried away by gravitons while energy is conserved in beta decay by the neutrino. These might be alternate ways of saying the same thing. 

 

The Role of Gravitation in Physics

Table of Contents

Preface

Acknowledgements

1 The Chapel Hill Conference in Context
Dean Rickles

2 The Authors

The Original Chapel Hill Report

Foreword
Cécile DeWitt

PARTICIPANTS IN THE CONFERENCE

Session I Unquantized General Relativity Chairman: B. S. DeWitt

3 The Present Position of Classical Relativity Theory and Some of its Problems
John Wheeler

4 The Experimental Basis of Einstein's Theory
R. H. Dicke

Session II Unquantized General Relativity, Continued
Chairman: P. G. Bergmann

5 On the Integration of the Einstein Equations
André Lichnerowicz

6 Remarks on Global Solutions
C. W. Misner

7 Solving The Initial Value Problem Using Cartan Calculus
Y. Fourès

8 Some Remarks on Cosmological Models
R. W. Bass, L. Witten

Session III Unquantized General Relativity, Continued
Chairman: H. Bondi

9 Gravitational Waves
L. Marder, Presented by H. Bondi

10 Gravitational Field of an Axially Symmetric System
N. Rosen, H. Shamir, Presented by F. Pirani

11 The Dynamics of a Lattice Universe
R. W. Lindquist

Session IV Invited Reports on Cosmology Chairman: F. J. Belinfante

12 Measurable Quantities that May Enable Questions of Cosmology to be Answered
Thomas Gold

13 Radio Astronomical Measurements of Interest to Cosmology
A. E. Lilley

Session V Unquantized General Relativity, Concluded
Chairman: A. Lichnerowicz

14 Measurement of Classical Gravitation Fields
Felix Pirani

15 Correspondence in the Generalized Theory of Gravitation
Behram Kursunoglu

16 Presentation of Work by T. Taniuchi
Ryoyu Utiyama

17 Negative Mass in General Relativity
Hermann Bondi

Session VI Quantized General Relativity Chairman: J. A. Wheeler

18 The Problems of Quantizing the Gravitational Field
P. G. Bergmann

19 Conceptual Clock Models
H. Salecker

20 The Three-Field Problem
F. J. Belinfante

Session VII Quantized General Relativity, Continued Chairman: A. Schild

21 Quantum Gravidynamics
Bryce DeWitt

Session VIII Quantized General Relativity, Concluded Chairman: V. Bargmann

22 The Possibility of Gravitational Quantization

23 The Necessity of Gravitational Quantization

Closing Session Chairman: B. S. DeWitt

24 Divergences in Quantized General Relativity
S. Deser

25 Critical Comments
R. P. Feynman

26 Summary of Conference
P. G. Bergmann

27 An Expanded Version of the Remarks by R.P. Feynman on the Reality of Gravitational Waves


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