
Graduate Course Descriptions - UC Berkeley Physics
... 231. General Relativity. (4) Three hours of lecture and one hour of discussion per week. Prerequisites: 209 or equivalent, or consent of instructor. An introduction to Einstein's theory of gravitation. Tensor analysis, general relativistic models for matter and electromagnetism, Einstein's field eq ...
... 231. General Relativity. (4) Three hours of lecture and one hour of discussion per week. Prerequisites: 209 or equivalent, or consent of instructor. An introduction to Einstein's theory of gravitation. Tensor analysis, general relativistic models for matter and electromagnetism, Einstein's field eq ...
Philosophy and Religion Studies / Physics • Courses
... waves; effective range theory; integral equation approach; resonances; bound states; variational and R-Matrix methods. Emphasis on applications. Prerequisite(s): PHYS 5510. 6161. Introduction to Scattering Theory II. 3 hours. Time-dependent potential scattering, the general theory of collisions, ele ...
... waves; effective range theory; integral equation approach; resonances; bound states; variational and R-Matrix methods. Emphasis on applications. Prerequisite(s): PHYS 5510. 6161. Introduction to Scattering Theory II. 3 hours. Time-dependent potential scattering, the general theory of collisions, ele ...
Quantum Field Theory, its Concepts Viewed from a Semiotic
... asymptotic particles subject to the strong interaction are supposed to be related to particular ‘products’ of these fields. This theoretical picture is called confinement and has not yet been deduced rigorously. But perturbation theory can be used under very restricted kinematical conditions, where ...
... asymptotic particles subject to the strong interaction are supposed to be related to particular ‘products’ of these fields. This theoretical picture is called confinement and has not yet been deduced rigorously. But perturbation theory can be used under very restricted kinematical conditions, where ...
Emergence, Reduction, and Theoretical Principles
... the properties of macroscopic material bodies we see that the whole becomes “not only more than but very different from the sum of its parts” (Anderson 1972, 395). The significance of the dependence on theoretical principles like SSB for the reductionist hypothesis is that results of the sort mentio ...
... the properties of macroscopic material bodies we see that the whole becomes “not only more than but very different from the sum of its parts” (Anderson 1972, 395). The significance of the dependence on theoretical principles like SSB for the reductionist hypothesis is that results of the sort mentio ...
Nonexistence of the Classical Trajectories in the Stern
... thus representing the noninteracting systems. Needless to say, then there is no room for the atomic R system to play the atomic CM system’s environment. Formally, as it can be easily shown, the state of the composite system CM + S + R is of the separable form |Ψ iCM+S |φiR , where |Ψ iCM+S is presen ...
... thus representing the noninteracting systems. Needless to say, then there is no room for the atomic R system to play the atomic CM system’s environment. Formally, as it can be easily shown, the state of the composite system CM + S + R is of the separable form |Ψ iCM+S |φiR , where |Ψ iCM+S is presen ...
What is Renormalization? G.Peter Lepage
... Although electron scattering on external fields has been fixed, we must worry about the effect of the new cutoff on other processes. Consider for example the one-loop corrections to electron-electron scattering (Fig. 2). The k > Λ contributions due to vertex and self-energy corrections to the one-ph ...
... Although electron scattering on external fields has been fixed, we must worry about the effect of the new cutoff on other processes. Consider for example the one-loop corrections to electron-electron scattering (Fig. 2). The k > Λ contributions due to vertex and self-energy corrections to the one-ph ...
The Cosmological Constant From The Viewpoint Of String Theory
... clue to understand particle physics better; if the cosmological constant must be treated anthropically – and the approximate vacuum we live in is drawn fortuitously from an ensemble – I am not optimistic about how well we will be able to understand the aspects of particle physics that are not expla ...
... clue to understand particle physics better; if the cosmological constant must be treated anthropically – and the approximate vacuum we live in is drawn fortuitously from an ensemble – I am not optimistic about how well we will be able to understand the aspects of particle physics that are not expla ...
Supersymmetric quantum mechanics and the Index Theorem
... which particles moving in a curved space-time (i.e. with external gauge and gravitational fields) will be massless. This could be for the direct reason that the degrees of freedom relevant to the presently known particle spectrum are truly massless, on the scale of some Planckian unification mass; o ...
... which particles moving in a curved space-time (i.e. with external gauge and gravitational fields) will be massless. This could be for the direct reason that the degrees of freedom relevant to the presently known particle spectrum are truly massless, on the scale of some Planckian unification mass; o ...
Particle Physics on Noncommutative Spaces
... • Lots of corrections to SM processes, but large background: search for rare decays. • Smoking gun for NC: Z--> or Z--> g g. • Limit on NC from LEP is below 1 TeV. ...
... • Lots of corrections to SM processes, but large background: search for rare decays. • Smoking gun for NC: Z--> or Z--> g g. • Limit on NC from LEP is below 1 TeV. ...
CHAPTER 15 - Quantum cryptography
... Or |11>. This means that subsequent measurement of other particle (on another planet) provides the same result as the measurement of the first particle. This indicate that in quantum world non-local influences, correlations exist. Quantum cryptography ...
... Or |11>. This means that subsequent measurement of other particle (on another planet) provides the same result as the measurement of the first particle. This indicate that in quantum world non-local influences, correlations exist. Quantum cryptography ...
The Evolution of Quantum Field Theory, From QED to Grand
... the only two force theories that are really successful, being electrodynamics and Einstein’s General Relativity, are both based on some fundamental local symmetry, are there other ways to employ symmetries in a similar way, to describe different forces? When I was M. Veltman’s undergraduate student, ...
... the only two force theories that are really successful, being electrodynamics and Einstein’s General Relativity, are both based on some fundamental local symmetry, are there other ways to employ symmetries in a similar way, to describe different forces? When I was M. Veltman’s undergraduate student, ...
Relativity and Quantum Mechanics
... experiments in free fall produce the same results as those of an inertial observer. Examples include if you are in an isolated lift cabin and drop an object, the object falls to the ground this could occur either as expected on earth, or in deep space, where gravity is zero, but frame is acceler ...
... experiments in free fall produce the same results as those of an inertial observer. Examples include if you are in an isolated lift cabin and drop an object, the object falls to the ground this could occur either as expected on earth, or in deep space, where gravity is zero, but frame is acceler ...
Quantum gravity

Quantum gravity (QG) is a field of theoretical physics that seeks to describe the force of gravity according to the principles of quantum mechanics.The current understanding of gravity is based on Albert Einstein's general theory of relativity, which is formulated within the framework of classical physics. On the other hand, the nongravitational forces are described within the framework of quantum mechanics, a radically different formalism for describing physical phenomena based on probability. The necessity of a quantum mechanical description of gravity follows from the fact that one cannot consistently couple a classical system to a quantum one.Although a quantum theory of gravity is needed in order to reconcile general relativity with the principles of quantum mechanics, difficulties arise when one attempts to apply the usual prescriptions of quantum field theory to the force of gravity. From a technical point of view, the problem is that the theory one gets in this way is not renormalizable and therefore cannot be used to make meaningful physical predictions. As a result, theorists have taken up more radical approaches to the problem of quantum gravity, the most popular approaches being string theory and loop quantum gravity. A recent development is the theory of causal fermion systems which gives quantum mechanics, general relativity, and quantum field theory as limiting cases.Strictly speaking, the aim of quantum gravity is only to describe the quantum behavior of the gravitational field and should not be confused with the objective of unifying all fundamental interactions into a single mathematical framework. While any substantial improvement into the present understanding of gravity would aid further work towards unification, study of quantum gravity is a field in it's own right with various branches having different approaches to unification. Although some quantum gravity theories, such as string theory, try to unify gravity with the other fundamental forces, others, such as loop quantum gravity, make no such attempt; instead, they make an effort to quantize the gravitational field while it is kept separate from the other forces. A theory of quantum gravity that is also a grand unification of all known interactions is sometimes referred to as a theory of everything (TOE).One of the difficulties of quantum gravity is that quantum gravitational effects are only expected to become apparent near the Planck scale, a scale far smaller in distance (equivalently, far larger in energy) than what is currently accessible at high energy particle accelerators. As a result, quantum gravity is a mainly theoretical enterprise, although there are speculations about how quantum gravity effects might be observed in existing experiments.