Quantum field theory is by far the most spectacularly successful theory in physics, but also one of the most mystifying. Quantum Field Theory, as Simply as Possible provides an essential primer on the subject, giving readers the conceptual foundations they need to wrap their heads around one of the most important yet baffling subjects in physics.
Quantum field theory grew out of quantum mechanics in the late 1930s and was developed by a generation of brilliant young theorists, including Julian Schwinger and Richard Feynman. Their predictions were experimentally verified to an astounding accuracy unmatched by the rest of physics. Quantum field theory unifies quantum mechanics and special relativity, thus providing the framework for understanding the quantum mysteries of the subatomic world. With his trademark blend of wit and physical insight, A. Zee guides readers from the classical notion of the field to the modern frontiers of quantum field theory, covering a host of topics along the way, including antimatter, Feynman diagrams, virtual particles, the path integral, quantum chromodynamics, electroweak unification, grand unification, and quantum gravity.
A unique and valuable introduction for students and general readers alike, Quantum Field Theory, as Simply as Possible explains how quantum field theory informs our understanding of the universe, and how it can shed light on some of the deepest mysteries of physics.
An exceptionally accessible introduction to quantum field theory
Quantum field theory is by far the most spectacularly successful theory in physics, but also one of the most mystifying. Quantum Field Theory, as Simply as Possible provides an essential primer on the subject, giving readers the conceptual foundations they need to wrap their heads around one of the most important yet baffling subjects in physics.
Quantum field theory grew out of quantum mechanics in the late 1930s and was developed by a generation of brilliant young theorists, including Julian Schwinger and Richard Feynman. Their predictions were experimentally verified to an astounding accuracy unmatched by the rest of physics. Quantum field theory unifies quantum mechanics and special relativity, thus providing the framework for understanding the quantum mysteries of the subatomic world. With his trademark blend of wit and physical insight, A. Zee guides readers from the classical notion of the field to the modern frontiers of quantum field theory, covering a host of topics along the way, including antimatter, Feynman diagrams, virtual particles, the path integral, quantum chromodynamics, electroweak unification, grand unification, and quantum gravity.
A unique and valuable introduction for students and general readers alike, Quantum Field Theory, as Simply as Possible explains how quantum field theory informs our understanding of the universe, and how it can shed light on some of the deepest mysteries of physics.
My popular book Quantum Field Theory, As Simply As Possible will be published by Princeton University Press on January 17, 2023. As a popular book, QFT ASAP is written especially for people who want to learn about quantum field theory but do not have the mathematical background to tackle my textbook Quantum Field Theory in a Nutshell. For some readers, it might serve as a stepping stone towards QFT Nut.
I find it counterproductive when people treat the formulation of relativistic QFTs as a matter of second quantization. It confuses learners into thinking that it involves going beyond the general principles of quantum theory. The real change is going from situations where the wave function formulation is often the most convenient (for non-relativistic situations) to a Heisenberg-picture formulation with heavy emphasis on its time-dependent operators.
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In textbooks this shows up as the fact that the Legendre transform from velocity to momentum variables is only one-to-one in special circumstances. Even for free field theories this becomes a problem, typically first seen when you try to quantize the theory of a free photon, and find that the canonical momentum for the time-like component of the vector field is zero.
This is simply not the case. You just use products of fields (not necessarily at the same space-time point) that have the quantum numbers to add or remove one of the bound state particles you are interested in. For example in QCD, if you want to find an S-matrix element or an operator matrix element involving protons, you would use a product of three fields for the up quark for an outgoing proton, and the hermitian conjugate field product for an incoming proton.
Then you apply the LSZ method unchanged.
That is, you examine Green functions that include these fields. In momentum space, corresponding to the bound state there is a pole in the external momentum of the field product. In coordinate space, there is the corresponding asymptotic large-time oscillatory behavior.
Essentially the same idea is used in lattice QCD to calculate matrix elements of operators between hadron states. The important difference is that instead of the oscillating asymptotic behavior in Minkowski coordinate space, one has exponential decay corresponding to the mass of the particle.
In this post I want to try and paint a picture of what it means to have a field that respects the laws of quantum mechanics. In a previous post, I introduced the idea of fields (and, in particular, the all-important electric field) by making an analogy with ripples on a pond or water spraying out from a hose. These images go surprisingly far in allowing one to understand how fields work, but they are ultimately limited in their correctness because the implied rules that govern them are completely classical. In order to really understand how nature works at its most basic level, one has to think about a field with quantum rules.
(By the way, this why physicists build huge particle accelerators whenever they want to study exotic heavy particles. If you want to create something heavy like the Higgs boson, you have to hit the Higgs field with a sufficiently large (and sufficiently concentrated) burst of energy to give the field the necessary one quantum of energy.)
The other big implication of imposing quantum rules on the ball-and-spring motion is that it changes pretty dramatically the meaning of empty space. Normally, empty space, or vacuum, is defined as the state where no particles are around. For a classical field, that would be the state where all the ball-and-springs are stationary and the field is flat. Something like this:
But in a quantum field, the ball-and-springs can never be stationary: they are always moving, even when no one has added enough energy to the field to create a particle. This means that what we call vacuum is really a noisy and densely energetic surface:
5. Also quantum field gives rise to different fluctuations which in turn gives rise to different elementary parts (matter field and force field). This means that each such variation and combination produces a different universe all together but all arising from the same vacuum field fluctuation.
There are sort of three problems with your alternate picture of a quantum field. The first is that it would allow any arbitrarily small amount of energy to be added to the field, as long as it remained in only one spring.
4) What information most succinctly defines a particle? Is it the point origin and amplitude? Is an "electron" simply an oscillation of (making this up) amplitude=5 at point X,Y in the field? How would you define an "electron"?
1) In the real universe, energy is neither created nor destroyed. It simply moves from one kind of field to another. You have to remember that the universe is filled with many different kinds of fields, all coexisting with each other and all having different kinds of properties. They can interact with each other, and when they do some ripples in one field are transferred to another.
4) This again comes down to a difference between different types of fields. One answer is that if you put in a single quantum of energy, you will get one particle unambiguously. But if your field has many quanta of energy in the field, then sometimes it is less clear. In the picture I drew here, you could imagine making a big disturbance of the field, and this could either have one ripple with large amplitude, or many ripples with small amplitude. (Keeping in mind that no individual wave can have less than one quantum of energy.) In technical language, one could say that the field created here does not conserve particle number (it is a bosonic field).
A single gold atom is already an intricate composite object, made of many separate excitations of different fields. What we call a gold atom is really 79 excitations of the electron field, 237 excitations of the quark fields, and countless excitations of the photon (electromagnetic) and gluon (strong force) fields. These excitations are doing sort of a dance where they all stick together. And the fact that a gold atom is stable means precisely that such a dance of many excitations is possible.
A simplified analogous example would be to consider a low resolution black and white monitor. Every possible permutations of different screens can be produced. Each screen is a picture of at least something, some where, some time in the universe at that definition. A valid theory should result in the ordering of these screens into a movie of the universe.
It is possible that Ectoe is a valid description of the universe inclusive of all other such possible universes. Even if this is not true Ectoe is perhaps otherwise the best science fiction ever Developed, condensed and expressed mathematically. The existence Constance is constrained to have a pair of real factors, each of which must be less than infinite and greater than zero. In this way existence is bounded between an outer limit like barrier of maximum existence potential and near the origin of near total kinetic existence. The theory suggesting a unique reflection of existence occurs at each barrier. However any movement back to the origin is difficult to detect having occurred at a location (inclusive of time) before the observer could note. We see the universe flying apart with a tendency to randomness. ECTOE is suggesting a kind of cyclic equilibrium returning order to the universe occurs for the next expansion event.
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