• Study Resource
  • Explore
    • Arts & Humanities
    • Business
    • Engineering & Technology
    • Foreign Language
    • History
    • Math
    • Science
    • Social Science

    Top subcategories

    • Advanced Math
    • Algebra
    • Basic Math
    • Calculus
    • Geometry
    • Linear Algebra
    • Pre-Algebra
    • Pre-Calculus
    • Statistics And Probability
    • Trigonometry
    • other →

    Top subcategories

    • Astronomy
    • Astrophysics
    • Biology
    • Chemistry
    • Earth Science
    • Environmental Science
    • Health Science
    • Physics
    • other →

    Top subcategories

    • Anthropology
    • Law
    • Political Science
    • Psychology
    • Sociology
    • other →

    Top subcategories

    • Accounting
    • Economics
    • Finance
    • Management
    • other →

    Top subcategories

    • Aerospace Engineering
    • Bioengineering
    • Chemical Engineering
    • Civil Engineering
    • Computer Science
    • Electrical Engineering
    • Industrial Engineering
    • Mechanical Engineering
    • Web Design
    • other →

    Top subcategories

    • Architecture
    • Communications
    • English
    • Gender Studies
    • Music
    • Performing Arts
    • Philosophy
    • Religious Studies
    • Writing
    • other →

    Top subcategories

    • Ancient History
    • European History
    • US History
    • World History
    • other →

    Top subcategories

    • Croatian
    • Czech
    • Finnish
    • Greek
    • Hindi
    • Japanese
    • Korean
    • Persian
    • Swedish
    • Turkish
    • other →
 
Profile Documents Logout
Upload
Unitary time evolution
Unitary time evolution

... This simple result has many profound consequences. For one, the state |ψi of a system is not an observable. Given a quantum system, there is no way to tell in what state |ψi it was prepared. If the state |ψi is known, the state can be “copied” by preparing another system. But it is impossible to co ...
Localized shocks Please share
Localized shocks Please share

... where c0 , c1 , c2 are constants that depend on the Hamiltonian. The norm is the operator (infinity) norm, and the bound is valid as long as the interactions decay exponentially (or faster) with distance. This bound implies that the radius of the operator can grow no faster than linearly, r[Z1 (tw ) ...
Chapter 2 Foundations I: States and Ensembles
Chapter 2 Foundations I: States and Ensembles

... which is deterministic. If we specify |ψ(0)i, the theory predicts the state |ψ(t)i at a later time. But on the other hand there is measurement, which is probabilistic. The theory does not make definite predictions about the measurement outcomes; it only assigns probabilities to the various alternati ...
The Basics of Quantum Physics: Introducing State Vectors
The Basics of Quantum Physics: Introducing State Vectors

Two constructions of quantum graphs and two types of
Two constructions of quantum graphs and two types of

... graphs defined via scattering matrices would appear to be losing some generality. In Section 3.3 we will argue that this is not so. On the other hand, in the case when the Laplace operator produces an energyindependent S-matrix, the matrix S has some very special properties (see Lemma 2.1 and precee ...
ON THE GENERAL FORM OF QUANTUM STOCHASTIC
ON THE GENERAL FORM OF QUANTUM STOCHASTIC

... and identity preserving, t (I) = I in the case of bounded K and L. In the next sections we de…ne a multidimensional analog of the quantum stochastic equation (1.10) and will show that the suggested general structure of its generator indeed follows just from the property of complete positivity of the ...
Qudits of composite dimension, mutually unbiased bases and
Qudits of composite dimension, mutually unbiased bases and

Application of the Sampling and Replication Operators to Describe
Application of the Sampling and Replication Operators to Describe

Holomorphic Methods in Mathematical Physics
Holomorphic Methods in Mathematical Physics

... This shows that the sequence Fm converges locally uniformly to some limit function, which must be F. (If L2 limit and pointwise limit both exist they must be equal a.e.) But a standard theorem shows that a locally uniform limit of holomorphic functions is always holomorphic. (Use Morera’s Theorem to ...
Theoretical aspects of Solid State Physics
Theoretical aspects of Solid State Physics

... physical problem may have an exact (or high precision) solution as, for example, in the case of spectrum of Hydrogen atom, or for a value of the fundamental constant e2 /h̄c. Typically, however, it is not so, because of two reasons: first, objects are too complicated in almost all cases and, second, ...
Hydrogen Atom.
Hydrogen Atom.

Kazakov - From Sigma Models to Four-dimensional QFT
Kazakov - From Sigma Models to Four-dimensional QFT

... • From action on matrix element ...
Can one distinguish quantum trees from the boundary?
Can one distinguish quantum trees from the boundary?

... attaching semi-infinite wires to all boundary vertices. Hence this matrix function encodes all information that can be obtained by boundary measurements. Extending the spectral data set further by including TW-functions associated with both boundary and internal vertices makes the inverse problem to ...
Dual Density Operators and Natural Language
Dual Density Operators and Natural Language

... Clearly, the use of a category of inner-product spaces and linear maps is not at all essential; it suffices to have any compact-closed category, or even more general, a category that matches the structure of the chosen categorial grammar [9]. Since the CPM-construction maps a dagger compact closed c ...
Transition probabilities and dynamic structure factor in the ASEP
Transition probabilities and dynamic structure factor in the ASEP

... stationary state, the time-dependent characteristics are very nontrivial to obtain, even in the simplest periodic one-dimensional case (closed ring of L sites). This is due to the fact that e.g. the time-dependent operators of type eHt fˆ(0)e−Ht are complicated objects because the generator of the s ...
Chapter 12 Path Integral for Fermion Fields
Chapter 12 Path Integral for Fermion Fields

... A → A + dΛ this functions transforms as Φ → Φ + Λ. Using the identity 2iΣαβ = γ α γ β − δ αβ one sees that ...
Lecture 2: Bogoliubov theory of a dilute Bose gas Abstract
Lecture 2: Bogoliubov theory of a dilute Bose gas Abstract

... for conservation of total particle number. We shall also carefully distinguish Bose-Einstein condensation from superfluidity. Interactions are necessary for superfluidity to take place. Interactions are not needed for Bose-Einstein condensation. From a technical point of view, we begin with the form ...
Quantum many-body systems exactly solved by special functions
Quantum many-body systems exactly solved by special functions

Entangled Simultaneous Measurement and Elementary Particle Representations
Entangled Simultaneous Measurement and Elementary Particle Representations

... elementary particle multiplets, Levine [18] suggested the generalization of spin (SU (2)) measurement to the measurement of SO(2n) Clifford algebra operators using 2n spin meters. A more fundamental application to elementary particle multiplets, originating in the structure of the Poincare algebra, ...
Lecture Notes for Ph219/CS219: Quantum Information and Computation Chapter 2 John Preskill
Lecture Notes for Ph219/CS219: Quantum Information and Computation Chapter 2 John Preskill

Chapter 4 MANY PARTICLE SYSTEMS
Chapter 4 MANY PARTICLE SYSTEMS

Symmetries of a system
Symmetries of a system

Frobenius-Perron Resonances for Maps with a Mixed Phase Space
Frobenius-Perron Resonances for Maps with a Mixed Phase Space

Observables and Measurements in Quantum Mechanics
Observables and Measurements in Quantum Mechanics

- Philsci
- Philsci

... Jauch’s criterion seems to suggest that, to obtain a wider theory, one should treat some intrinsic properties of the particle as extrinsic. But this would be in vain unless it had a surplus of physical meaning. De Muynck (1975) remarks on Jauch’s criterion, ”an intrinsic property may show up dynamic ...
< 1 ... 7 8 9 10 11 12 13 14 15 ... 32 >

Self-adjoint operator

  • studyres.com © 2025
  • DMCA
  • Privacy
  • Terms
  • Report