• Study Resource
  • Explore Categories
    • 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
The Ensembles
The Ensembles

The Equivalence Myth of Quantum Mechanics
The Equivalence Myth of Quantum Mechanics

CHAPTER 4 RIGID-ROTOR MODELS AND ANGULAR MOMENTUM
CHAPTER 4 RIGID-ROTOR MODELS AND ANGULAR MOMENTUM

PowerPoint
PowerPoint

Adiabatic State Preparation of Interacting Two-Level Systems R. T. Brierley, C. Creatore,
Adiabatic State Preparation of Interacting Two-Level Systems R. T. Brierley, C. Creatore,

... Discrete atomic-like systems, or qubits, can be excited by using external field pulses that induce Rabi oscillations, with the final state determined by the intensity and duration of the pulse. However, this method is sensitive to fluctuations in the driving field, transition energy and other source ...
An Entropy Approach to the Natures of the Electric Charge and
An Entropy Approach to the Natures of the Electric Charge and

Unlocking the Lagrangian.
Unlocking the Lagrangian.

... a given location. If we want to know where a system is heading, we add its current state to its potential, right? Sounds feasible, but that isn't what is happening. The Lagrangian isn't a sum of present and future, it is a sum of energy due to charge and energy due to gravity. As with Newton's gravi ...
PowerPoint
PowerPoint

Plasma Physics / Course Content
Plasma Physics / Course Content

Atomic quantum phase studies with a longitudinal Stern
Atomic quantum phase studies with a longitudinal Stern



quantum computation of the jones polynomial - Unicam
quantum computation of the jones polynomial - Unicam

Monday, Mar. 28, 2005
Monday, Mar. 28, 2005

Exact diagonalization of quantum spin models
Exact diagonalization of quantum spin models

Spontaneous persistent currents in a quantum spin Hall insulator D. Soriano
Spontaneous persistent currents in a quantum spin Hall insulator D. Soriano

Carbon – Science and Technology
Carbon – Science and Technology

... electromagnetics/transport dynamics in realistic environments. It is highlighted that the selfgenerated electromagnetic field may affect the dynamics (group velocity, kinetic energy etc.) of the quantum transport. This is particularly important in the analysis of time transients and in the describin ...
PH504lec0809-4
PH504lec0809-4

... the electric dipole. The electric dipole - definition Consists of two equal and opposite charges Q separated by a distance s. In an ideal dipole s is very small compared to the distances to any other charges and also to any points where we wish to find the resultant electric potential or E-field. H ...
Eigenstate Phase Transitions
Eigenstate Phase Transitions

Course Competency Learning Outcomes
Course Competency Learning Outcomes

PH 213 ENERGY CONSERVATION The Fisrt Law of
PH 213 ENERGY CONSERVATION The Fisrt Law of

Tip-Enhanced Fluorescence Microscopy at 10 Nanometer Resolution
Tip-Enhanced Fluorescence Microscopy at 10 Nanometer Resolution

... was insufficient to differentiate between various models because they did not probe the high-contrast region within several nanometers of tip-sample contact. The measured z  a6 decay corresponds to the ‘‘near-field’’ term in the expression for the field intensity near a point dipole, where z is ...
Lecture 8
Lecture 8

QUANTUM DYNAMICS OF A MASSLESS RELATIVISTIC
QUANTUM DYNAMICS OF A MASSLESS RELATIVISTIC

... that the ends of the string move at the speed of light. Another is the fact that only the motion of the string perpendicular to itself is dynamically significant. Thus the number of independent vibrations of the string is only two: the string is transverse. The string can then be quantized by making ...
Computation of hadronic two-point functions in Lattice QCD
Computation of hadronic two-point functions in Lattice QCD

Consciousness, the Brain, and Spacetime Geometry
Consciousness, the Brain, and Spacetime Geometry

< 1 ... 268 269 270 271 272 273 274 275 276 ... 822 >

T-symmetry

  • studyres.com © 2026
  • DMCA
  • Privacy
  • Terms
  • Report