Chapter 1 - UniMAP Portal
Chapter 1 - UniMAP Portal

Decay Widths and Scattering Cross Sections
Decay Widths and Scattering Cross Sections

Relatives of the quotient of the complex projective plane by complex
Relatives of the quotient of the complex projective plane by complex

... nionic-linear transformation, preserving the hyperhermitian structure. (A quaternioniclinear operator is a linear operator A, for which A(qx) = qA(x) for any quaternion q). The dimension of the hyperunitary group of the hyperhermitian space Hm equals m(2m + 1). This group is denoted (unfortunatly) S ...
Fall 2012 Midterm Answers.
Fall 2012 Midterm Answers.

topic 1 - Dr. Mohd Afendi Bin Rojan, CEng MIMechE
topic 1 - Dr. Mohd Afendi Bin Rojan, CEng MIMechE

L1-2. Special Matrix Operations: Permutations, Transpose, Inverse
L1-2. Special Matrix Operations: Permutations, Transpose, Inverse

S How to Generate Random Matrices from the Classical Compact Groups
S How to Generate Random Matrices from the Classical Compact Groups

4_PCA
4_PCA

Lecture 11a
Lecture 11a

Motion Relative to a non-inertial frame
Motion Relative to a non-inertial frame

Lecture 5 Group actions
Lecture 5 Group actions

1 Inner product spaces
1 Inner product spaces

CLASS 12 MATHEMATICS SAMPLE PAPER – 1 SECTION – A
CLASS 12 MATHEMATICS SAMPLE PAPER – 1 SECTION – A

LINEAR TRANSFORMATIONS AND THEIR
LINEAR TRANSFORMATIONS AND THEIR

Relativistic effects in the dynamical Casimir effect
Relativistic effects in the dynamical Casimir effect

... • In Fig. 1, we notice the rising of a second band of created particles in the spectral distribution when the velocity of the effective mirror can achieved 10% of the speed of light. The inset highlight the assymetric shape of the second band. The ratio between the peak of the second and first bands ...
1. Grassmann Bundles. Note if you have a smooth embedded curve
1. Grassmann Bundles. Note if you have a smooth embedded curve

THE FUNDAMENTAL THEOREM OF ALGEBRA VIA LINEAR ALGEBRA
THE FUNDAMENTAL THEOREM OF ALGEBRA VIA LINEAR ALGEBRA

THE FUNDAMENTAL THEOREM OF ALGEBRA VIA LINEAR
THE FUNDAMENTAL THEOREM OF ALGEBRA VIA LINEAR

Matrices to work with intersections of equations of planes
Matrices to work with intersections of equations of planes

Lecture 1 - GEOCITIES.ws
Lecture 1 - GEOCITIES.ws

A write-up on the combinatorics of the general linear group
A write-up on the combinatorics of the general linear group

Slide 1
Slide 1

On Finding the Characteristic Equation of a Square Matrix
On Finding the Characteristic Equation of a Square Matrix

Slide 1
Slide 1

Some Linear Algebra Notes
Some Linear Algebra Notes

Four-vector

In the theory of relativity, a four-vector or 4-vector is a vector in Minkowski space, a four-dimensional real vector space. It differs from a Euclidean vector in how its magnitude is determined. The transformations that preserve this magnitude are the Lorentz transformations, which include spatial rotations, boosts (a change by a constant velocity to another inertial reference frame), and temporal and spatial inversions. Regarded as a homogeneous space, the transformation group of Minkowski space is the Poincaré group, which adds to the Lorentz group the group of translations. The Lorentz group may be represented by 4×4 matrices.The article considers four-vectors in the context of special relativity. Although the concept of four-vectors also extends to general relativity, some of the results stated in this article require modification in general relativity.