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Math Test

Inline

  • Metric: gμν
  • Derivative: μϕ
  • Einstein eq.: Gμν=8πGTμν
  • FRW: ds2=dt2+a(t)2dx2

Display

gμν=diag(1,1,1,1)μTμν=0S=d4xg[R16πG12gμνμϕνϕV(ϕ)]

Aligned equations

H2=(a˙a)2=8πG3ρH˙=4πG(ρ+p)

Fractions, roots, sums

01x2dx=13,1+ϵ1+ϵ2,n=11n2=π26

Greek + accents

α,β,γ,Γ,Λ,Ω,ϕ˙, ϕ¨, g~μν, ρ¯

text boxes

Definition: Phase Space

A phase space is the set of all possible states of a process or system at a specific time. For a mechanical system with n degrees of freedom, the phase space is typically 2n-dimensional, parameterized by coordinates and momenta (qi,pi).

Example: Simple Harmonic Oscillator

For a simple 1D harmonic oscillator, the state is determined by its position x and velocity v. The phase space is the 2D plane with coordinates (x,v). The system's evolution is described by:

dxdt=v,dvdt=ω2x

The phase curves are ellipses centered at the origin.

Theorem: Liouville's Theorem

For a Hamiltonian system, the phase-space volume is preserved along the flow of the system. If ρ(q,p,t) is the probability density function in phase space, then:

dρdt=ρt+i=1n(ρqiq˙i+ρpip˙i)=0

Important Remark: Singularities

When analyzing phase flows, special care must be taken near equilibrium points where the vector field vanishes (i.e., v(x)=0). Trajectories can take infinite time to reach these critical points.