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The Road to Reality : A Complete Guide to the Laws of the Universe Hardcover – February 22, 2005
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Since the earliest efforts of the ancient Greeks to find order amid the chaos around us, there has been continual accelerated progress toward understanding the laws that govern our universe. And the particularly important advances made by means of the revolutionary theories of relativity and quantum mechanics have deeply altered our vision of the cosmos and provided us with models of unprecedented accuracy.
What Roger Penrose so brilliantly accomplishes in this book is threefold. First, he gives us an overall narrative description of our present understanding of the universe and its physical behaviors–from the unseeable, minuscule movement of the subatomic particle to the journeys of the planets and the stars in the vastness of time and space.
Second, he evokes the extraordinary beauty that lies in the mysterious and profound relationships between these physical behaviors and the subtle mathematical ideas that explain and interpret them.
Third, Penrose comes to the arresting conclusion–as he explores the compatibility of the two grand classic theories of modern physics–that Einstein’s general theory of relativity stands firm while quantum theory, as presently constituted, still needs refashioning.
Along the way, he talks about a wealth of issues, controversies, and phenomena; about the roles of various kinds of numbers in physics, ideas of calculus and modern geometry, visions of infinity, the big bang, black holes, the profound challenge of the second law of thermodynamics, string and M theory, loop quantum gravity, twistors, and educated guesses about science in the near future. In The Road to Reality he has given us a work of enormous scope, intention, and achievement–a complete and essential work of science
- Print length1136 pages
- LanguageEnglish
- PublisherKnopf
- Publication dateFebruary 22, 2005
- Dimensions6.63 x 2.23 x 9.44 inches
- ISBN-100679454438
- ISBN-13978-0679454434
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“A truly remarkable book...Penrose does much to reveal the beauty and subtlety that connects nature and the human imagination, demonstrating that the quest to understand the reality of our physical world, and the extent and limits of our mental capacities, is an awesome, never-ending journey rather than a one-way cul-de-sac.”
—London Sunday Times
“Penrose’s work is genuinely magnificent, and the most stimulating book I have read in a long time.”
—Scotland on Sunday
“Science needs more people like Penrose, willing and able to point out the flaws in fashionable models from a position of authority and to signpost alternative roads to follow.”
—The Independent
“What a joy it is to read a book that doesn't simplify, doesn't dodge the difficult questions, and doesn't always pretend to have answers...Penrose’s appetite is heroic, his knowledge encyclopedic, his modesty a reminder that not all physicists claim to be able to explain the world in 250 pages.”
—London Times
“For physics fans, the high point of the year will undoubtedly be The Road to Reality.”
—Guardian
About the Author
Excerpt. © Reprinted by permission. All rights reserved.
The purpose of this book is to convey to the reader some feeling for what is surely one of the most important and exciting voyages of discovery that humanity has embarked upon. This is the search for the underlying principles that govern the behaviour of our universe. It is a voyage that has lasted for more than two-and-a-half millennia, so it should not surprise us that substantial progress has at last been made. But this journey has proved to be a profoundly difficult one, and real understanding has, for the most part, come but slowly. This inherent difficulty has led us in many false directions; hence we should learn caution. Yet the 20th century has delivered us extraordinary new insights–some so impressive that many scientists of today have voiced the opinion that we may be close to a basic understanding of all the underlying principles of physics. In my descriptions of the current fundamental theories, the 20th century having now drawn to its close, I shall try to take a more sober view. Not all my opinions may be welcomed by these ‘optimists’, but I expect further changes of direction greater even than those of the last century.
The reader will find that in this book I have not shied away from presenting mathematical formulae, despite dire warnings of the severe reduction in readership that this will entail. I have thought seriously about this question, and have come to the conclusion that what I have to say cannot reasonably be conveyed without a certain amount of mathematical notation and the exploration of genuine mathematical concepts. The understanding that we have of the principles that actually underlie the behaviour of our physical world indeed depends upon some appreciation of its mathematics. Some people might take this as a cause for despair, as they will have formed the belief that they have no capacity for mathematics, no matter at how elementary a level. How could it be possible, they might well argue, for them to comprehend the research going on at the cutting edge of physical theory if they cannot even master the manipulation of fractions? Well, I certainly see the difficulty.
Yet I am an optimist in matters of conveying understanding. Perhaps I am an incurable optimist. I wonder whether those readers who cannot manipulate fractions–or those who claim that they cannot manipulate fractions–are not deluding themselves at least a little, and that a good proportion of them actually have a potential in this direction that they are not aware of. No doubt there are some who, when confronted with a line of mathematical symbols, however simply presented, can see only the stern face of a parent or teacher who tried to force into them a non-comprehending parrot-like apparent competence–a duty, and a duty alone–and no hint of the magic or beauty of the subject might be allowed to come through. Perhaps for some it is too late; but, as I say, I am an optimist and I believe that there are many out there, even among those who could never master the manipulation of fractions, who have the capacity to catch some glimpse of a wonderful world that I believe must be, to a significant degree, genuinely accessible to them.
One of my mother’s closest friends, when she was a young girl, was among those who could not grasp fractions. This lady once told me so herself after she had retired from a successful career as a ballet dancer. I was still young, not yet fully launched in my activities as a mathematician, but was recognized as someone who enjoyed working in that subject. ‘It’s all that cancelling’, she said to me, ‘I could just never get the hang of cancelling.’ She was an elegant and highly intelligent woman, and there is no doubt in my mind that the mental qualities that are required in comprehending the sophisticated choreography that is central to ballet are in no way inferior to those which must be brought to bear on a mathematical problem. So, grossly overestimating my expositional abilities, I attempted, as others had done before, to explain to her the simplicity and logical nature of the procedure of ‘cancelling’.
I believe that my efforts were as unsuccessful as were those of others. (Incidentally, her father had been a prominent scientist, and a Fellow of the Royal Society, so she must have had a background adequate for the comprehension of scientific matters. Perhaps the ‘stern face’ could have been a factor here, I do not know.) But on reflection, I now wonder whether she, and many others like her, did not have a more rational hang-up–one that with all my mathematical glibness I had not noticed. There is, indeed, a profound issue that one comes up against again and again in mathematics and in mathematical physics, which one first encounters in the seemingly innocent operation of cancelling a common factor from the numerator and denominator of an ordinary numerical fraction.
Those for whom the action of cancelling has become second nature, because of repeated familiarity with such operations, may find themselves insensitive to a difficulty that actually lurks behind this seemingly simple procedure. Perhaps many of those who find cancelling mysterious are seeing a certain profound issue more deeply than those of us who press onwards in a cavalier way, seeming to ignore it. What issue is this? It concerns the very way in which mathematicians can provide an existence to their mathematical entities and how such entities may relate to physical reality.
I recall that when at school, at the age of about 11, I was somewhat taken aback when the teacher asked the class what a fraction (such as 3/8) actually is! Various suggestions came forth concerning the dividing up of pieces of pie and the like, but these were rejected by the teacher on the (valid) grounds that they merely referred to imprecise physical situations to which the precise mathematical notion of a fraction was to be applied; they did not tell us what that clear-cut mathematical notion actually is. Other suggestions came forward, such as 3/8 is ‘something with a 3 at the top and an 8 at the bottom with a horizontal line in between’ and I was distinctly surprised to find that the teacher seemed to be taking these suggestions seriously! I do not clearly recall how the matter was finally resolved, but with the hindsight gained from my much later experiences as a mathematics undergraduate, I guess my schoolteacher was making a brave attempt at telling us the definition of a fraction in terms of the ubiquitous mathematical notion of an equivalence class.
What is this notion? How can it be applied in the case of a fraction and tell us what a fraction actually is? Let us start with my classmate’s ‘something with a 3 at the top and an 8 on the bottom’. Basically, this is suggesting to us that a fraction is specified by an ordered pair of whole numbers, in this case the numbers 3 and 8. But we clearly cannot regard the fraction as being such an ordered pair because, for example, the fraction 6/16 is the same number as the fraction 3/8, whereas the pair (6, 16) is certainly not the same as the pair (3, 8). This is only an issue of cancelling; for we can write 6/16 as 3x2/8x2 and then cancel the 2 from the top and the bottom to get 3/8. Why are we allowed to do this and thereby, in some sense, ‘equate’ the pair (6, 16) with the pair (3, 8)? The mathematician’s answer–which may well sound like a cop-out–has the cancelling rule just built in to the definition of a fraction: a pair of whole numbers (a x n, b x n) is deemed to represent the same fraction as the pair (a, b) whenever n is any non-zero whole number (and where we should not allow b to be zero either).
But even this does not tell us what a fraction is; it merely tells us something about the way in which we represent fractions. What is a fraction, then? According to the mathematician’s ‘‘equivalence class’’ notion, the fraction 3/8, for example, simply is the infinite collection of all
pairs
(3, 8), ( – 3, – 8), (6, 16), ( – 6, – 16), (9, 24), ( – 9, – 24), (12, 32), . . . ,
where each pair can be obtained from each of the other pairs in the list by repeated application of the above cancellation rule.* [ * This is called an ‘equivalence class’ because it actually is a class of entities (the entities, in this particular case, being pairs of whole numbers), each member of which is deemed to be equivalent, in a specified sense, to each of the other members.] We also need definitions telling us how to add, subtract, and multiply such infinite collections of pairs of whole numbers, where the normal rules of algebra hold, and how to identify the whole numbers themselves as particular types of
fraction.
This definition covers all that we mathematically need of fractions (such as 1/2 being a number that, when added to itself, gives the number 1, etc.), and the operation of cancelling is, as we have seen, built into the definition. Yet it seems all very formal and we may indeed wonder whether it really captures the intuitive notion of what a fraction is. Although this ubiquitous equivalence class procedure, of which the above illustration is just a particular instance, is very powerful as a pure-mathematical tool for establishing consistency and mathematical existence, it can provide us with very topheavy-looking entities. It hardly conveys to us the intuitive notion of what 3/8 is, for example! No wonder my mother’s friend was confused.
In my descriptions of mathematical notions, I shall try to avoid, as far as I can, the kind of mathematical pedantry that leads us to define a fraction in terms of an ‘infinite class of pairs’ even though it certainly has its value in mathematical rigour and precision. In my descriptions here I shall be more concerned with conveying the id...
Product details
- Publisher : Knopf (February 22, 2005)
- Language : English
- Hardcover : 1136 pages
- ISBN-10 : 0679454438
- ISBN-13 : 978-0679454434
- Item Weight : 3.3 pounds
- Dimensions : 6.63 x 2.23 x 9.44 inches
- Best Sellers Rank: #223,990 in Books (See Top 100 in Books)
- #281 in Cosmology (Books)
- #362 in Astrophysics & Space Science (Books)
- #1,815 in Mathematics (Books)
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Here is a summary of what I have found out to be very applicable and useful:
(1) p.7: What laws govern our universe? How shall we know them? How may this knowledge help us to comprehend the world any hence guide its actions to our advantage? ... Eventually, even the much more complicated apparent motions of the planets began to yield up their secrets, revealing an immerse underlying precision and regularity.
(2) p.18: Fig. 1.3 Three 'worlds' - the Platonic mathematical, the physical, and the mental - and the three profound mysteries in the connections between them. ... everything in the physical universe is indeed governed in completely precise detail by mathematical principles. ... all actions in the universe could be entirely subject to mathematical laws.
(3) p.28: Euclid's first postulate effectively asserts that there is a (unique) straight line segment connecting any two points. His second postulate asserts the unlimited (continuous) extendibility of any straight line segment. His third postulate asserts the existence of a circle with any centre and with any value for its radius. Finally, his fourth postulate asserts the equality of all right angles.
(4) p.45: We are to think of a light, straight, stiff rod, at one end P of which is attached a heavy point-like weight, and the other end R moves along the asymptote.
(5) p.67: The system of complex numbers is an even more striking instance of the convergence between mathematical ideas and the deeper workings of the physical universe.
(6) p. 109: What about the places where the second derivative f''(x) meets the x-axis? These occur where the curvature of f(x) vanishes. In general, these points are where the direction in which the curve y = f(x) 'bends' changes from one side to the other, at a place called a point of inflection.
(7) p. 115: Armed with these few rules (and loads and loads of practice), one can become an 'expert' at differentiation without needing to have much in the way of actual understanding of why the rules work! This is the power of a good calculus.
(8) p.151: Air, of course, consists of enormous numbers of individual fundamental particles (in fact, about 10^20 of them in a cubic centimeter), so airflow is something whose macroscopic description involves a considerable amount of averaging and approximation. There is no reason to expect that the mathematical equations of aerodynamics should reflect a great deal of the mathematics that is deeply involved in the physical laws that govern those individual particles.
(9) p. 211: It seems that Nature assigns a different role to each of these two reduced spin-spaces, and it is through this fact physical processes that are reflection non-invariant can emerge. It was, indeed, one of the most striking unprecedented discoveries of 20th-century physics (theoretically predicted by Chen Ning Yang and Tsung Dao Lee, and experimentally confirmed by Chien-Shiung Wu and her group, in 1957) that there are actually fundamental processes in Nature which do not occur in their mirror-reflected form.
(10) p. 217: For example, the configuration space of an ordinary rigid body in Euclidean 3-space is a non-Euclidean 6-manifold.
(11) p.223: As in Sec 10.2, we have the notion of a smooth function (Phi), defined on manifold M.
(12) p.388: He (Newton) had originally proposed five (or six) laws, law 4 of which was indeed the Galilean principle, but later he simplified them, in his published Principia, to the three 'Newton's laws that we are now familiar with.
(13) p. 390: It is remarkable that, from just these simple ingredients (Newton's formula GmM/r^2), a theory of extraordinary power and versatility arises, which can be used with great accuracy to describe the behavior of macroscopic bodies (and, for most basic considerations, submicroscopic particles also), so long as their speeds are significantly less than that of light.,
(14) p. 392: Galileo's insight does not apply to electric forces; it is a particular feature of gravity alone.
(15) p. 410: We shall also begin to witness the extraordinary power, beauty, and accuracy of Einstein's revolutionary theory.
(16) p. 412: The geometries of Euclidean 2-space and 3-space are very familiar to us. Moreover, the generalization to a 4-dimensional Euclidean geometry E^4 is not difficult to make in principle, although it is not something for which 'visual intuition' can be appealed to.
(17) p. 455: Einstein's famous equation E = mc^2 tells us that mass and energy are basically the same thing and, as Newton had already informed us, it is mass that is the source of gravitation.
(18) p. 462: Einstein originally introduced this extra term, in order to have the possibility of a static spatially closed universe on the cosmological scale. But when it became clear, from Edwin Hubble's observations in 1929, that the universe is expanding, and therefore not static, Einstein withdrew his support for this cosmological constant, asserting that it had been 'his greatest mistake' (perhaps because he might otherwise have predicted the expansion of the universe!). Nevertheless, ideas once put forward do not necessarily go away easily. The cosmological constant has hovered in the background of cosmological theory ever since Einstein first put it forward, causing worry to some and solace to others. Very recently, observations of distant supernovae have had most theorists to re-introduce /\ (greek lambda), or something similar, referred to as 'dark energy', as a way of making these observations consistent with other perceived requirements.
(19) p. 466: The timing of these signals is so precise, and the system itself so 'clean', that comparison between observation and theoretical expectation provides a confirmation of Einstein's general relativity to about one part in 10^14, an accuracy unprecedented in the scientific comparison between the observation of a particular system and theory.
(20) p.490: He (Hilbert) appears to have believed that his total Lagrangian gives us what we would now refer to as a 'theory of everything'.
(21) p. 503: ... it took many years for Einstein's original lonely insights to become accepted.
(22) p. 523: Heisenberg's uncertainty relation tells us that the product of these two spreads cannot be smaller than the order of Planck's constant, and we have Delta-p Delat-x >= h_bar / 2.
(23) p. 528: I denote Schrodinger evolution by U and state reduction by R. This alternation between these two completely different-looking procedures would appear to be a distinctly odd type of way for a universe to behave!
(24) p. 541: As the state of the arts stands, one can either be decidedly sloppy about such mathematical niceties and even pretend that position states and momentum states are actually states, or else spend the whole time insisting on getting the mathematics right, in which case there is a contrasting danger of getting trapped in a 'rigour mortis.'
(25) p.686 (Chapter 27 The Big Bang and its Thermodynamic Legacy): What sorts of laws shape the universe with all its contents? The answer provided by practically all successful physical theories, from the time of Galileo onwards, would be given in the form of a dynamics - that is, a specification of how a physical system will develop with time, given the physical state of of the system at one particular time. These theories do not tell us what the world is like; they say, instead: 'if the world was like such-and-such at one time, then it will be like so-and-so at some later time'.
(26) p.687: The usual way of thinking about how these dynamical laws act is that it is the choice of initial conditions that determines which particular realization of the dynamics happens to occur. Normally, one thinks in terms of systems evolving into the future, from data specified in the last, where the particular evolution that takes place is determined by differential equations.
(27) p.689: What about evolution into the past, rather than the future? It would be a fair comment that such 'chaotic unpredictability" is normally much worse for the 'retrodiction' that is involved in past-directed evolution than for the 'prediction' of the normal future-directed evolution. This has to do with the Second Law of thermodynamics, which in its simplest form basically asserts: Heat flows from a hotter to a cooler body. ... This procedure of dynamic retrodiction is clearly a hopeless prospect in physics. ... For this kind of reason, physics is normally concerned with prediction, rather than retrodiction.
(28) p. 760: Of course, it might indeed ultimately turn out that there is simply no mathematical way of fixing certain parameters in the 'true theory', and that the choice of these parameters is indeed such that the universe in which we find ourselves must be so as to allow sentient life. But I have to confess that I do not much like that idea!
(29) p. 850: But to take this position is to part company with one of the basic principles of Einstein's theory, namely the principle of general covariance.
(30) p. 935: ... A lot of these stem from the fact Einstein's theory is 'generally covariant' (Sec 19.6).
Finally, I have to say that I really like so many drawings in the book, which are simplistic yet stupendously expressive. Thanks Professor Penrose for sharing your knowledge and achievements of many decades, which will benefit many on this planet called Earth!
Several distinguished features of this book include:
1. more than 1000 pages with neither typos nor grammatical errors.
2. almost all major roads to final theory: string theory, loop variables, twistor theory, non-commutative geometry. For descriptions, the book deals with classical mechanics, relativity, quantum mechanics, and chaos theory from the basics. And also it deals with classical and modern mathematics: irrational numbers, Euclidean geometry, hyperbolic geometry, projective geometry, real number calculus, complex number calculus, Riemann surfaces, Fourier decomposition, generalized functions, Clifford algebra, Grassmann algebra, vector fields on manifolds, Riemannian geometry, exterior derivative, Lie groups, Lie algebras, connections, fibre bundle theory, Cantor's set theory, Minkowskian geometry, Lorentz geometry, sheaf theory, and tensors. But in spirit, this book is for general audience.
What is the most important for a reader? I think it is how much he learned from the reading. In this aspect, I could not give five stars. To finish the book, I spent almost two months. Of course, I learned a quite amount and it was a valuable time. But I think what I gained is just 35 percent of what the book contains. Comparing with Brian Green's popular books, the book is the next or the next-next level of a book. The difficulty was in concepts relating to relativity, in particular, tensors. In the book, the tensor notation is universal. Even the Maxwell equation is expressed in the tensor notation. I graduated in physics department and have a doctoral degree in mathematics. But I've never studied general relativity and its related Lorenz and Minkowskian geometry, and tensor notations. And I've never studied quantum field theory and its related tensor formalism as well.
If you think that the book is difficult for you also, I would like to give some tips. They are all related to skipping.
1. As the author says, skip equations and difficult parts if you don't want to read it sometimes the whole chapter. If you realize that the part is important to understand the main stream of the book, you can always go back to that part when necessary. At page 74, the author says,
My advice to such readers is basically just to read the words and not to bother too much about trying to understand the equations.
2. This book is not a textbook. If you want to learn relativity or tensor calculus or quantum physics, then you are referred to standard texts or Youtube lectures. You should not try to learn such subjects from this book. So when you meet some parts dealing with such a sophisticated level physics and think that it's too difficult, you should skip it without any regret.
3. As I said, in spirit, the book is for general audience. But if one can understand more than a half of the book, then I think that he would be at least a graduate student studying quantum field theory and relativity. If you are interested in the question, what laws govern our universe, you are entitled to read the book. But actually, if you are not already familiar with quantum mechanics at least at the level of popular science books, then it would be extremely hard for you to read. You have to make clever choices about what to read if you don't want to spend time frustrated.
4. Its style is informal and narrative, but in some parts, it is very dense. For example, the Newton mechanics is summarized only in three pages. After the section, the author assumes that you have mastered the Newton mechanics!
Now I want to share my detailed appreciation.
1. If your major is related to science, then among many curriculum subjects, the linear algebra would be the most helpful to read this book, such as, basis, eigenvalue, linear transformations and matrices, basis change, dimension of a vector space. And if you know what a phase space is for a dynamical system, then it would be very helpful (Search the Wiki). And if your major is mathematics, I have something more to say. I've read the differential geometry book by O'Neil, Calculus on Manifolds by Spivak and studied one-semester courses of differential topology and Riemannian geometry. So I am familiar with concepts like curvature, 1-form, integration on forms, exterior derivative, Poincare lemma. But that was not so helpful to understand relativity and tensors in the book. Everybody who is interested in the subject knows that they are related, but I think that they live somewhat in different area.
2. The book is so concise that sometimes you can't understand what the author says. For example, I think that the Mach-Zehnder interferometer at page 514 cannot be understood only by the explanations of the book if the reader does not already know it. And for many extremely important experiments including EPR-experiment, the book describes them so briefly that if you are not already familiar with them, you may have difficulty to understand them. And as for quantum entanglement, it is a really amazing phenomenon of quantum mechanics. But if you didn't already know it, then you may not fully understand it only with this book. As one more example of physics part, while I read the book, I come to know that there is a projective postulate in quantum mechanics that seems to be a very important issue in the book. But I couldn't understand it even though I tried to read the related parts several times. There are such things on the mathematical part. First of all, although there are explanations about tensors, if you are not already familiar with it, you would have a rare chance of understanding it. As the second instance, at the extremely interesting section on covariant derivative on a fibre bundle (Section 15.8), the explanation is not sufficient for actually calculating the example of A=ik the conjugate of z. As another instance, in the sections on complex numbers, we see some logically vague explanations. I found that the author didn't explain the fact that if two holomorphic functions on a domain D coincide on a continuous set (in a sense), then they coincide on the domain D.
3. There seem to be unsatisfactory explanations. At section 14.3, introducing covariant derivative, the author introduces the concept of parallel transport. But there is some ambiguity whether covariant derivative is derived from the parallel transport or the converse is true (this case is true in mathematical literature). And at section 21.4, it explains the Blackbody radiation. Wien's formula was already there giving insufficient interpretation of Blackbody radiation and several years after Wien, Planck succeeded in explaining Blackbody radiation with introducing his Planck constant. If so, it is absurd that the Planck constant appears in the Wien's formula.
4. If you are a mathematician, I strongly recommend that you read sections on analytic continuation, hyper-functions, Fourier decomposition, fibre bundles. They are worth reading in the aspect that the book explains to readers the geometric meaning. Once you read them, you will not forget it for a long time. For example, we know that a conformal map is an angle preserving map. The author says that a conformal map preserves shape locally. Maybe this is a common sense to many researchers, but to me it was an astonishing insight. There are many things like that in the book. And there are some differences of point of view to mathematicians like me. For example, in Chapter 5, the author explains complex numbers from the basics, and in Chapter 13, symmetry groups. I thought I knew them. But the way he describes them seems to be strange. As for complex numbers, I skipped some parts and made a decision to retain my understanding. As for symmetry groups, I thought I have to learn more.
5. Until the author introduces the generalized function, he asks us what function is. What definition of a function can be satisfactory in theoretical meaning and in practical applications? In fact, I used to ask the same question also, although I was not so explicit. I think anyone who studied mathematics for several years may have conceived the question. His argument is very interesting and really thought-provoking. More than that, he gives an explicit answer about the question.
6. Diagrammatic notations and conformal diagrams don't seem to be helpful for non-specialists.
7. While reading through the book, I hoped that I could understand the following sentence.
... according to modern physics, all physical interactions are governed by 'gauge connections' which, technically, depend crucially on spaces having exact symmetries. (page 289)
But even now after finishing the book, I still don't understand what the above sentence means concretely. My future goal would be to understand it.
8. What are the merits of the book? Does the book have a merit that other books do not have? I think it has. The author has no hesitation in expressing his explicit opinion about major current theories.
Quantum field theory - mathematically inconsistent
Inflation cosmology - suspicious
String theory - Doubtful, especially due to its higher-dimensional spacetime. String theory regards spacetime as continuum but the author seems to believe that ultimately, spacetime also should be quantized.
Loop variables - At this stage, it is far from being quantum gravity theory.
Non-commutative geometry - The model does not incorporate special and general relativity.
Quantum group - There is no very clear relation between a quantum group and quantum theory.
Topological quantum field theory - It is hard to see them playing direct roles as models of serious physical theories.
Another merit of the book is that it gave me a motivation to study relativity, tensors, and quantum field theory by showing a big picture of modern attempts to final theory. I am a group theorist, and I want to meet more various groups in physics. And I am interested in the question: what laws govern our universe? This is the motivation that I chose the book. I hope that I learn more about the area. As remarked above, ultimately, the spacetime also seems that it should have a discrete property at extremely small scale. So some scientists suggested a discrete number system other than real numbers. I thought that's the right way! But the author suggests that rather than a discrete number system, complex number system would be the right number system. Now I think that it is possible that to describe a discrete object, we may use a continuum like the complex number system.
As a whole, the reading was valuable. While I read this book, I received the impression that the author is a very gentle, sincere, honest, kind, careful, and friendly person. Even though I was not totally satisfied with the book, I come to respect his attitude as a scholar.
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