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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{Quantum book backlink|Quantum field theory}}&lt;br /&gt;
Quantum field theory basics: particles as excitations of fields, spacetime, Feynman diagrams, and gauge symmetries.&amp;lt;br&amp;gt;Quantum field theory describes particles as excitations of underlying fields, combining quantum mechanics with special relativity to explain particle interactions and fundamental forces.&amp;lt;ref&amp;gt;{{cite book |last=Peskin |first=Michael E. |year=1995}}&amp;lt;/ref&amp;gt;&amp;lt;div style=&amp;quot;float:right; border:1px solid #ccc; padding:4px; background:#fff8dc; margin:0 0 1em 1em; width:420px;&amp;quot;&amp;gt;&lt;br /&gt;
[[File:Quantum_field_theory_basics1.jpg]]&lt;br /&gt;
&amp;lt;div style=&amp;quot;font-size:90%;&amp;quot;&amp;gt;Overview of key concepts in quantum field theory&amp;lt;/div&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=Creation/annihilation operators=&lt;br /&gt;
&lt;br /&gt;
In quantum field theory, particles are described as excitations of underlying fields. The creation and annihilation operators provide a mathematical framework for adding or removing particles from a system.&amp;lt;ref&amp;gt;{{cite book |last=Peskin |first=Michael E. |last2=Schroeder |first2=Daniel V. |title=An Introduction to Quantum Field Theory |publisher=Westview Press |year=1995}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Definition ===&lt;br /&gt;
&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;annihilation operator&amp;#039;&amp;#039;&amp;#039; &amp;lt;math&amp;gt;\hat{a}_k&amp;lt;/math&amp;gt; removes a particle from a mode with momentum &amp;lt;math&amp;gt;k&amp;lt;/math&amp;gt;, while the &amp;#039;&amp;#039;&amp;#039;creation operator&amp;#039;&amp;#039;&amp;#039; &amp;lt;math&amp;gt;\hat{a}_k^\dagger&amp;lt;/math&amp;gt; adds a particle:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\hat{a}_k |n_k\rangle = \sqrt{n_k}\,|n_k - 1\rangle,&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\hat{a}_k^\dagger |n_k\rangle = \sqrt{n_k+1}\,|n_k + 1\rangle.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Commutation relations ===&lt;br /&gt;
&lt;br /&gt;
For bosons, the operators satisfy&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
[\hat{a}_k, \hat{a}_{k&amp;#039;}^\dagger] = \delta_{kk&amp;#039;}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For fermions, they satisfy anticommutation relations:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\{\hat{a}_k, \hat{a}_{k&amp;#039;}^\dagger\} = \delta_{kk&amp;#039;}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Field expansion ===&lt;br /&gt;
&lt;br /&gt;
A quantum field can be written as a sum over modes:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\phi(x) = \sum_k \left( \hat{a}_k u_k(x) + \hat{a}_k^\dagger u_k^*(x) \right).&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This expresses the field as a superposition of particle creation and annihilation processes.&lt;br /&gt;
&lt;br /&gt;
=== Physical significance ===&lt;br /&gt;
&lt;br /&gt;
Creation and annihilation operators:&lt;br /&gt;
&lt;br /&gt;
* describe particle number changes,  &lt;br /&gt;
* allow treatment of multi-particle systems,  &lt;br /&gt;
* form the basis of quantum field quantization.&lt;br /&gt;
&lt;br /&gt;
=Fock space=&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Fock space&amp;#039;&amp;#039;&amp;#039; is the Hilbert space used in quantum field theory to describe systems with a variable number of particles. It is constructed as a direct sum of multi-particle spaces built from single-particle states.&amp;lt;ref&amp;gt;{{cite book |last=Peskin |first=Michael E. |last2=Schroeder |first2=Daniel V. |title=An Introduction to Quantum Field Theory |publisher=Westview Press |year=1995}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Definition ===&lt;br /&gt;
&lt;br /&gt;
Fock space is defined as&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\mathcal{F} = \mathbb{C} \oplus \mathcal{H} \oplus (\mathcal{H} \otimes \mathcal{H}) \oplus \cdots,&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\mathcal{H}&amp;lt;/math&amp;gt; is the single-particle Hilbert space.&lt;br /&gt;
&lt;br /&gt;
Each term represents states with:&lt;br /&gt;
&lt;br /&gt;
* 0 particles (vacuum),  &lt;br /&gt;
* 1 particle,  &lt;br /&gt;
* 2 particles,  &lt;br /&gt;
* and so on.  &lt;br /&gt;
&lt;br /&gt;
=== Vacuum state ===&lt;br /&gt;
&lt;br /&gt;
The vacuum state &amp;lt;math&amp;gt;|0\rangle&amp;lt;/math&amp;gt; contains no particles and satisfies&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\hat{a}_k |0\rangle = 0.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
All other states are built by applying creation operators to the vacuum.&lt;br /&gt;
&lt;br /&gt;
=== Multi-particle states ===&lt;br /&gt;
&lt;br /&gt;
A general multi-particle state is constructed as&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
|n_1, n_2, \dots\rangle = \prod_k \frac{(\hat{a}_k^\dagger)^{n_k}}{\sqrt{n_k!}} |0\rangle.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This describes a configuration with &amp;lt;math&amp;gt;n_k&amp;lt;/math&amp;gt; particles in each mode.&lt;br /&gt;
&lt;br /&gt;
=== Bosons and fermions ===&lt;br /&gt;
&lt;br /&gt;
The structure of Fock space depends on particle statistics:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Bosons&amp;#039;&amp;#039;&amp;#039; — symmetric states (no restriction on occupation number)  &lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Fermions&amp;#039;&amp;#039;&amp;#039; — antisymmetric states (Pauli exclusion principle: &amp;lt;math&amp;gt;n_k = 0 \text{ or } 1&amp;lt;/math&amp;gt;)  &lt;br /&gt;
&lt;br /&gt;
=== Physical significance ===&lt;br /&gt;
&lt;br /&gt;
Fock space:&lt;br /&gt;
&lt;br /&gt;
* allows description of systems with changing particle number,  &lt;br /&gt;
* provides the natural setting for quantum fields,  &lt;br /&gt;
* is essential in particle physics and quantum many-body theory.&lt;br /&gt;
&lt;br /&gt;
=Propagators=&lt;br /&gt;
&lt;br /&gt;
In quantum field theory, a &amp;#039;&amp;#039;&amp;#039;propagator&amp;#039;&amp;#039;&amp;#039; describes the probability amplitude for a particle to travel from one spacetime point to another. It plays a central role in calculations of particle interactions and quantum processes.&amp;lt;ref&amp;gt;{{cite book |last=Peskin |first=Michael E. |last2=Schroeder |first2=Daniel V. |title=An Introduction to Quantum Field Theory |publisher=Westview Press |year=1995}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Definition ===&lt;br /&gt;
&lt;br /&gt;
For a scalar field, the propagator is given by the time-ordered product&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
D(x - y) = \langle 0 | T\{\phi(x)\phi(y)\} | 0 \rangle,&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;T&amp;lt;/math&amp;gt; denotes time ordering.&lt;br /&gt;
&lt;br /&gt;
This quantity represents the amplitude for a particle created at point &amp;lt;math&amp;gt;y&amp;lt;/math&amp;gt; to be annihilated at point &amp;lt;math&amp;gt;x&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
=== Momentum-space form ===&lt;br /&gt;
&lt;br /&gt;
In momentum space, the propagator for a free scalar field has the form&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
\tilde{D}(p) = \frac{1}{p^2 - m^2 + i\epsilon}.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The small imaginary term &amp;lt;math&amp;gt;i\epsilon&amp;lt;/math&amp;gt; ensures proper boundary conditions and causality.&lt;br /&gt;
&lt;br /&gt;
=== Interpretation ===&lt;br /&gt;
&lt;br /&gt;
Propagators encode how disturbances in a field propagate through spacetime. They are not classical trajectories, but quantum amplitudes that contribute to observable processes.&lt;br /&gt;
&lt;br /&gt;
=== Role in interactions ===&lt;br /&gt;
&lt;br /&gt;
In interacting theories, propagators appear as internal lines in [[Feynman diagram|Feynman diagrams]]. They connect interaction vertices and represent virtual particles.&lt;br /&gt;
&lt;br /&gt;
=== Physical significance ===&lt;br /&gt;
&lt;br /&gt;
Propagators:&lt;br /&gt;
&lt;br /&gt;
* describe the propagation of particles and fields,  &lt;br /&gt;
* are fundamental building blocks of quantum field theory,  &lt;br /&gt;
* enable calculation of scattering amplitudes and correlation functions.&lt;br /&gt;
&lt;br /&gt;
=Feynman diagrams=&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Feynman diagrams&amp;#039;&amp;#039;&amp;#039; are graphical representations of interactions between particles in quantum field theory. They provide an intuitive and systematic way to calculate probability amplitudes for physical processes.&amp;lt;ref&amp;gt;{{cite book |last=Peskin |first=Michael E. |last2=Schroeder |first2=Daniel V. |title=An Introduction to Quantum Field Theory |publisher=Westview Press |year=1995}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
=== Basic elements ===&lt;br /&gt;
&lt;br /&gt;
A Feynman diagram consists of:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;External lines&amp;#039;&amp;#039;&amp;#039; — incoming and outgoing particles  &lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Internal lines&amp;#039;&amp;#039;&amp;#039; — propagators (virtual particles)  &lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Vertices&amp;#039;&amp;#039;&amp;#039; — interaction points  &lt;br /&gt;
&lt;br /&gt;
Each element corresponds to a mathematical expression in perturbation theory.&lt;br /&gt;
&lt;br /&gt;
=== Example ===&lt;br /&gt;
[[File:Electron-positron-scattering.svg|thumb|300px|Example of a Feynman diagram: electron–photon scattering. Straight lines represent fermions, wavy lines represent photons, and vertices represent interactions.]]&lt;br /&gt;
A simple interaction, such as electron–photon scattering, can be represented by a diagram where:&lt;br /&gt;
&lt;br /&gt;
* straight lines represent fermions,  &lt;br /&gt;
* wavy lines represent photons,  &lt;br /&gt;
* vertices represent electromagnetic interactions.&lt;br /&gt;
&lt;br /&gt;
=== Perturbation theory ===&lt;br /&gt;
&lt;br /&gt;
Feynman diagrams arise from expanding the evolution operator in powers of the interaction strength. Each diagram corresponds to a term in this expansion.&lt;br /&gt;
&lt;br /&gt;
The total amplitude is obtained by summing over all relevant diagrams.&lt;br /&gt;
&lt;br /&gt;
=== Feynman rules ===&lt;br /&gt;
&lt;br /&gt;
Each quantum field theory has a set of &amp;#039;&amp;#039;&amp;#039;Feynman rules&amp;#039;&amp;#039;&amp;#039; that translate diagrams into mathematical expressions:&lt;br /&gt;
&lt;br /&gt;
* propagators correspond to internal lines,  &lt;br /&gt;
* interaction terms determine vertex factors,  &lt;br /&gt;
* external lines correspond to particle states.  &lt;br /&gt;
&lt;br /&gt;
These rules allow systematic computation of scattering amplitudes.&lt;br /&gt;
&lt;br /&gt;
=== Virtual particles ===&lt;br /&gt;
&lt;br /&gt;
Internal lines represent &amp;#039;&amp;#039;&amp;#039;virtual particles&amp;#039;&amp;#039;&amp;#039;, which do not satisfy the usual energy–momentum relation:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;&lt;br /&gt;
p^2 \ne m^2.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
They are not directly observable but contribute to measurable quantities.&lt;br /&gt;
&lt;br /&gt;
=== Physical significance ===&lt;br /&gt;
&lt;br /&gt;
Feynman diagrams:&lt;br /&gt;
&lt;br /&gt;
* provide a visual representation of particle interactions,  &lt;br /&gt;
* simplify complex calculations in quantum field theory,  &lt;br /&gt;
* are essential in particle physics and high-energy experiments.  &lt;br /&gt;
&lt;br /&gt;
They are one of the most powerful tools for connecting theory with experimental predictions.&lt;br /&gt;
&lt;br /&gt;
==Further reading==&lt;br /&gt;
=== General readers===&lt;br /&gt;
* {{cite book|&lt;br /&gt;
last1=Pais|first1=A.|author-link1=Abraham Pais&lt;br /&gt;
|title=Inward Bound: Of Matter and Forces in the Physical World&lt;br /&gt;
|edition=reprint&lt;br /&gt;
|year=1994&lt;br /&gt;
|orig-date=1986&lt;br /&gt;
|publisher=[[Oxford University Press]]&lt;br /&gt;
|location=Oxford, New York, Toronto&lt;br /&gt;
|isbn=978-0-19-851997-3&lt;br /&gt;
}}&lt;br /&gt;
* {{cite book&lt;br /&gt;
|last=Schweber&lt;br /&gt;
|first=S. S.&lt;br /&gt;
|author-link=S. S. Schweber&lt;br /&gt;
|title=QED and the Men Who Made It: Dyson, Feynman, Schwinger, and Tomonaga&lt;br /&gt;
|year=1994&lt;br /&gt;
|isbn=978-0-691-03327-3&lt;br /&gt;
|url=https://archive.org/details/qedmenwhomadeitd0000schw&lt;br /&gt;
|publisher=[[Princeton University Press]]&lt;br /&gt;
|url-access=registration&lt;br /&gt;
}}&lt;br /&gt;
* {{cite book&lt;br /&gt;
 |last=Feynman &lt;br /&gt;
 |first=R.P.&lt;br /&gt;
 |year=2001&lt;br /&gt;
 |orig-date=1964&lt;br /&gt;
 |title=The Character of Physical Law&lt;br /&gt;
 |publisher=[[MIT Press]]&lt;br /&gt;
 |isbn=978-0-262-56003-0&lt;br /&gt;
 }}&lt;br /&gt;
* {{cite book |last=Feynman |first=R.P.&lt;br /&gt;
 |year=2006 |orig-date=1985&lt;br /&gt;
 |title=QED: The Strange Theory of Light and Matter&lt;br /&gt;
 |publisher=Princeton University Press&lt;br /&gt;
 |isbn=978-0-691-12575-6&lt;br /&gt;
}}&lt;br /&gt;
* {{cite book &lt;br /&gt;
 |last=Gribbin &lt;br /&gt;
 |first=J.     &lt;br /&gt;
 |author=John Gribbin]]&lt;br /&gt;
 |year=1998&lt;br /&gt;
 |title=Q is for Quantum: Particle Physics from A to Z&lt;br /&gt;
 |publisher=[[Weidenfeld &amp;amp; Nicolson]]&lt;br /&gt;
 |isbn=978-0-297-81752-9&lt;br /&gt;
}}&lt;br /&gt;
* {{Cite book |title=The Biggest Ideas in the Universe: quanta and fields |last=Carroll |first=Sean |publisher=[[E. P. Dutton]] |year=2024 |isbn=978-0-593-18660-2 |author=Sean M. Carroll}}&lt;br /&gt;
&lt;br /&gt;
=== Introductory texts===&lt;br /&gt;
&lt;br /&gt;
* {{cite book |author=Pierre van Baal |title=A Course in Field Theory |url=https://www.taylorfrancis.com/books/oa-mono/10.1201/b15364/course-field-theory-pierre-van-baal |isbn=978-0-429-07360-1 |year=2016 |publisher=[[CRC Press]] |doi=10.1201/b15364 }}&lt;br /&gt;
* {{cite book&lt;br /&gt;
  |last1=Cabibbo&lt;br /&gt;
  |first1=Nicola&lt;br /&gt;
  |last2=Maiani&lt;br /&gt;
  |first2=Luciano&lt;br /&gt;
  |last3=Benhar&lt;br /&gt;
  |first3=Omar&lt;br /&gt;
  |title=An Introduction to Gauge Theories&lt;br /&gt;
  |publisher=[[CRC Press]]&lt;br /&gt;
  |year=2025&lt;br /&gt;
  |doi=10.1201/9781003560708&lt;br /&gt;
 |isbn=9781003560708&lt;br /&gt;
  |url=https://doi.org/10.1201/9781003560708&lt;br /&gt;
}}&lt;br /&gt;
* {{cite book |last=Frampton |first=P.H. |author-link=Paul Frampton&lt;br /&gt;
 |year=2000&lt;br /&gt;
 |title=Gauge Field Theories&lt;br /&gt;
 |edition=2nd&lt;br /&gt;
 |series=Frontiers in Physics&lt;br /&gt;
 |publisher=[[John Wiley &amp;amp; Sons|Wiley]]&lt;br /&gt;
}}; {{cite book|title=2008, 3rd edition|url=https://books.google.com/books?id=AwhkM6hVj-wC|isbn=978-3-527-40835-1 | last1=Frampton | first1=Paul H. | date=22 September 2008 | publisher=John Wiley &amp;amp; Sons }}&lt;br /&gt;
* {{cite book |last1=Greiner |first1=W. |author-link=Walter Greiner |last2=Müller |first2=B.|author-link2=Berndt Müller&lt;br /&gt;
 |year=2000&lt;br /&gt;
 |title=Gauge Theory of Weak Interactions&lt;br /&gt;
 |publisher=[[Springer Science+Business Media|Springer]]&lt;br /&gt;
 |isbn=978-3-540-67672-0&lt;br /&gt;
}}&lt;br /&gt;
* {{cite book |last1=Itzykson |first1=C. |author-link=Claude Itzykson |last2=Zuber |first2=J.-B.|author-link2=Jean-Bernard Zuber&lt;br /&gt;
 |year=1980&lt;br /&gt;
 |title=Quantum Field Theory&lt;br /&gt;
 |url=https://archive.org/details/quantumfieldtheo0000itzy&lt;br /&gt;
 |url-access=registration&lt;br /&gt;
 |publisher=[[McGraw-Hill]]&lt;br /&gt;
 |isbn=978-0-07-032071-0&lt;br /&gt;
}}&lt;br /&gt;
* {{cite book |last=Kane |first=G.L. |author-link=Gordon L. Kane&lt;br /&gt;
 |year=1987&lt;br /&gt;
 |title=Modern Elementary Particle Physics&lt;br /&gt;
 |publisher=[[Perseus Books Group|Perseus Group]]&lt;br /&gt;
 |isbn=978-0-201-11749-3&lt;br /&gt;
}}&lt;br /&gt;
* {{cite book&lt;br /&gt;
 |last1=Kleinert&lt;br /&gt;
 |first1=H.&lt;br /&gt;
 |author-link=Hagen Kleinert&lt;br /&gt;
 |last2=Schulte-Frohlinde&lt;br /&gt;
 |first2=Verena&lt;br /&gt;
 |year=2001&lt;br /&gt;
 |title=Critical Properties of &amp;amp;phi;&amp;lt;sup&amp;gt;4&amp;lt;/sup&amp;gt;-Theories&lt;br /&gt;
 |url=http://users.physik.fu-berlin.de/~kleinert/re.html#B6&lt;br /&gt;
 |publisher=[[World Scientific]]&lt;br /&gt;
 |isbn=978-981-02-4658-7&lt;br /&gt;
 |archive-date=2012-07-22&lt;br /&gt;
 |access-date=2009-07-02&lt;br /&gt;
 |archive-url=https://web.archive.org/web/20120722013148/http://users.physik.fu-berlin.de/~kleinert/re.html#B6&lt;br /&gt;
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* {{cite book&lt;br /&gt;
 |last=Kleinert&lt;br /&gt;
 |first=H.&lt;br /&gt;
 |year=2008&lt;br /&gt;
 |title=Multivalued Fields in Condensed Matter, Electrodynamics, and Gravitation&lt;br /&gt;
 |url=http://users.physik.fu-berlin.de/~kleinert/public_html/kleiner_reb11/psfiles/mvf.pdf&lt;br /&gt;
 |publisher=World Scientific&lt;br /&gt;
 |isbn=978-981-279-170-2&lt;br /&gt;
 |archive-date=2012-07-16&lt;br /&gt;
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* {{Cite book |last1=Lancaster |first1=Tom&lt;br /&gt;
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 |url=https://books.google.com/books?id=Y-0kAwAAQBAJ&lt;br /&gt;
 |title=Quantum field theory for the gifted amateur&lt;br /&gt;
 |date=2014&lt;br /&gt;
 |publisher=Oxford University Press&lt;br /&gt;
 |isbn=978-0-19-969933-9&lt;br /&gt;
 |location=Oxford |oclc=859651399}}&lt;br /&gt;
* {{cite book |last=Loudon |first=R. |author-link=Rodney Loudon&lt;br /&gt;
 |year=1983&lt;br /&gt;
 |title=The Quantum Theory of Light&lt;br /&gt;
 |publisher=Oxford University Press&lt;br /&gt;
 |isbn=978-0-19-851155-7&lt;br /&gt;
}}&lt;br /&gt;
* {{cite book |last1=Maiani |first1=Luciano |author-link1=Luciano Maiani&lt;br /&gt;
 |last2=Benhar |first2=Omar&lt;br /&gt;
 |year=2024&lt;br /&gt;
 |title=Relativistic Quantum Mechanics: An Introduction to Relativistic Quantum Fields&lt;br /&gt;
 |publisher=CRC Press&lt;br /&gt;
 |isbn=9781003436263&lt;br /&gt;
 |url=https://doi.org/10.1201/9781003436263&lt;br /&gt;
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* {{cite book |last1=Mandl |first1=F. |author-link=Franz Mandl (physicist)&lt;br /&gt;
 |last2=Shaw |first2=G.&lt;br /&gt;
 |year=1993&lt;br /&gt;
 |title=Quantum Field Theory&lt;br /&gt;
 |publisher=[[John Wiley &amp;amp; Sons]]&lt;br /&gt;
 |isbn=978-0-471-94186-6 &lt;br /&gt;
}}&lt;br /&gt;
* {{cite book |last=Ryder |first=L.H. |author-link=Lewis Ryder&lt;br /&gt;
 |year=1985&lt;br /&gt;
 |title=Quantum Field Theory&lt;br /&gt;
 |url=https://books.google.com/books?id=nnuW_kVJ500C&lt;br /&gt;
 |publisher=[[Cambridge University Press]]&lt;br /&gt;
 |isbn=978-0-521-33859-2&lt;br /&gt;
}}&lt;br /&gt;
* {{cite book&lt;br /&gt;
 |last=Schwartz&lt;br /&gt;
 |first=M.D.&lt;br /&gt;
 |year=2014&lt;br /&gt;
 |title=Quantum Field Theory and the Standard Model&lt;br /&gt;
 |url=http://www.schwartzqft.com&lt;br /&gt;
 |publisher=Cambridge University Press&lt;br /&gt;
 |isbn=978-1-107-03473-0&lt;br /&gt;
 |access-date=2020-05-13&lt;br /&gt;
 |archive-url=https://web.archive.org/web/20180322014256/http://schwartzqft.com/&lt;br /&gt;
 |archive-date=2018-03-22&lt;br /&gt;
 }}&lt;br /&gt;
* {{cite book |last=Ynduráin |first=F.J. |author-link=Francisco José Ynduráin&lt;br /&gt;
 |year=1996&lt;br /&gt;
 |title=Relativistic Quantum Mechanics and Introduction to Field Theory&lt;br /&gt;
 |edition=1st&lt;br /&gt;
 |publisher=Springer&lt;br /&gt;
 |doi=10.1007/978-3-642-61057-8 |isbn=978-3-540-60453-2&lt;br /&gt;
|bibcode=1996rqmi.book.....Y }}&lt;br /&gt;
* {{cite book|last1=Greiner|first1=W.|author-link1=Walter Greiner&lt;br /&gt;
|last2=Reinhardt|first2=J.&lt;br /&gt;
|year=1996&lt;br /&gt;
|title=Field Quantization&lt;br /&gt;
|url=https://archive.org/details/fieldquantizatio0000grei|url-access=registration|publisher=Springer&lt;br /&gt;
|isbn=978-3-540-59179-5&lt;br /&gt;
}}&lt;br /&gt;
* {{cite book |last1=Peskin |first1=M. |author-link=Michael Peskin |last2=Schroeder |first2=D.&lt;br /&gt;
 |year=1995&lt;br /&gt;
 |title=An Introduction to Quantum Field Theory&lt;br /&gt;
 |url=https://books.google.com/books?id=i35LALN0GosC&lt;br /&gt;
 |publisher=[[Westview Press]]&lt;br /&gt;
 |isbn=978-0-201-50397-5&lt;br /&gt;
}}&lt;br /&gt;
* {{cite book|last=Scharf|first=Günter&lt;br /&gt;
|title=Finite Quantum Electrodynamics: The Causal Approach&lt;br /&gt;
|edition=third|year=2014&lt;br /&gt;
|orig-date=1989&lt;br /&gt;
|isbn=978-0-486-49273-5&lt;br /&gt;
|publisher=Dover Publications&lt;br /&gt;
}}&lt;br /&gt;
* {{cite book |last1=Srednicki |first1=M.&lt;br /&gt;
 |title=Quantum Field Theory&lt;br /&gt;
 |publisher=[[Cambridge University Press]]&lt;br /&gt;
 |year=2007&lt;br /&gt;
 |isbn=978-0521-8644-97&lt;br /&gt;
 |url=http://www.cambridge.org/us/catalogue/catalogue.asp?isbn=0521864496&lt;br /&gt;
}}&lt;br /&gt;
* {{cite web|last1=Tong |first1=David |author-link=David Tong (physicist)&lt;br /&gt;
|title=Lectures on Quantum Field Theory&lt;br /&gt;
|year=2015&lt;br /&gt;
|url=https://www.damtp.cam.ac.uk/user/tong/qft.html&lt;br /&gt;
|access-date=2016-02-09&lt;br /&gt;
}}&lt;br /&gt;
* {{cite book&lt;br /&gt;
 |last=Williams&lt;br /&gt;
 |first=A.G.&lt;br /&gt;
 |title=Introduction to Quantum Field Theory: Classical Mechanics to Gauge Field Theories&lt;br /&gt;
 |volume=&lt;br /&gt;
 |publisher=[[Cambridge University Press]]&lt;br /&gt;
 |year=2022&lt;br /&gt;
 |isbn=978-1-108-47090-2&lt;br /&gt;
 |url-access=&lt;br /&gt;
 |url=&lt;br /&gt;
 }}&lt;br /&gt;
* {{cite book&lt;br /&gt;
|last1=Zee&lt;br /&gt;
|first1=Anthony&lt;br /&gt;
|author-link=Anthony Zee&lt;br /&gt;
|title=Quantum Field Theory in a Nutshell&lt;br /&gt;
|edition=2nd&lt;br /&gt;
|year=2010&lt;br /&gt;
|isbn=978-0-691-14034-6&lt;br /&gt;
|publisher=[[Princeton University Press]]&lt;br /&gt;
|url-access=registration&lt;br /&gt;
|url=https://archive.org/details/isbn_9780691140346&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
=== Advanced texts===&lt;br /&gt;
&lt;br /&gt;
* Umezawa, H. (1956) &amp;#039;&amp;#039;Quantum Field Theory.&amp;#039;&amp;#039; North Holland Puplishing.&lt;br /&gt;
* Barton, G. (1963). &amp;#039;&amp;#039;Introduction to Advanced Field Theory.&amp;#039;&amp;#039; Intescience Publishers. &lt;br /&gt;
* {{cite book |last=Brown&lt;br /&gt;
 |first=Lowell S.&lt;br /&gt;
 |author-link=Lowell S. Brown&lt;br /&gt;
 |title=Quantum Field Theory&lt;br /&gt;
 |publisher=[[Cambridge University Press]]&lt;br /&gt;
 |year=1994&lt;br /&gt;
 |isbn=978-0-521-46946-3 &lt;br /&gt;
}}&lt;br /&gt;
* {{cite book |last1=Bogoliubov |first1=N.&lt;br /&gt;
 |last2=Logunov |first2=A.A. |author-link2=Anatoly Logunov&lt;br /&gt;
 |last3=Oksak |first3=A.I.&lt;br /&gt;
 |last4=Todorov |first4=I.T.&lt;br /&gt;
 |year=1990&lt;br /&gt;
 |title=General Principles of Quantum Field Theory&lt;br /&gt;
 |publisher=[[Kluwer Academic Publishers]]&lt;br /&gt;
 |isbn=978-0-7923-0540-8&lt;br /&gt;
}}&lt;br /&gt;
* {{cite book&lt;br /&gt;
 |last=Weinberg&lt;br /&gt;
 |first=S.&lt;br /&gt;
 |author-link=Steven Weinberg&lt;br /&gt;
 |title=The Quantum Theory of Fields&lt;br /&gt;
 |volume=1&lt;br /&gt;
 |publisher=[[Cambridge University Press]]&lt;br /&gt;
 |year=1995&lt;br /&gt;
 |isbn=978-0-521-55001-7&lt;br /&gt;
 |url-access=registration&lt;br /&gt;
 |url=https://archive.org/details/quantumtheoryoff00stev&lt;br /&gt;
 }}&lt;br /&gt;
* {{cite book |last1=Badger |first1=Simon |last2=Henn |first2=Johannes |last3=Plefka |first3=Jan Christoph |last4=Zoia |first4=Simone |title=Scattering Amplitudes in Quantum Field Theory |year=2024 |isbn=978-3-031-46987-9 |url=https://link.springer.com/book/10.1007/978-3-031-46987-9 |publisher=Springer |doi=10.1007/978-3-031-46987-9 |bibcode=2024saqf.book.....B }}&lt;br /&gt;
&lt;br /&gt;
=See also=&lt;br /&gt;
{{#invoke:PhysicsQC|tocHeadingAndList|Physics:Quantum basics/See also}}&lt;br /&gt;
&lt;br /&gt;
=References=&lt;br /&gt;
{{reflist|3}}&lt;br /&gt;
&lt;br /&gt;
{{Author|Harold Foppele}}&lt;br /&gt;
&lt;br /&gt;
{{Sourceattribution|Quantum field theory (QFT) basics|1}}&lt;/div&gt;</summary>
		<author><name>imported&gt;WikiHarold</name></author>
	</entry>
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