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Geometric Times: Clocks of Spacetime Metric

“Geometric time can be understood as the metric’s projection onto the observer.”

🎯 Core Proposition

In general relativity, “time” has multiple geometric realizations. In the GLS theoretical framework, they are classified as the unified time scale equivalence class :

Time TypeDefinitionApplicable Scenarios
Killing Time is a Killing vectorStatic spacetimes
ADM Lapse decomposition
Null Affine Parameter Null geodesics
Conformal Time FRW universe

Theoretical Proposition: Under appropriate conditions, these times are related to each other through affine transformations:

Thus mathematically belonging to the same equivalence class .

graph TB
    T["Unified Time Scale<br/>[τ]"] --> K["Killing Time<br/>t_K"]
    T --> A["ADM Time<br/>N·t"]
    T --> L["null parameter<br/>λ"]
    T --> E["Conformal Time<br/>η"]
    T --> M["Modular Time<br/>s_mod"]

    K -.->|"affine transformation"| A
    A -.->|"affine transformation"| L
    L -.->|"affine transformation"| E

    style T fill:#fff4e1,stroke:#ff6b6b,stroke-width:4px

💡 Intuitive Image: Rhythms of Different Clocks

Analogy: Multiple Clocks

Imagine a scenario:

  • Ground Clock: Second hand rotates uniformly (Killing time)
  • Mountain Clock: Faster at higher altitudes (ADM lapse)
  • Photon Clock: Massless, moves infinitely fast (null parameter)
  • Cosmic Clock: Slows down with cosmic expansion (conformal time)

They all serve as measures of time, but with different rhythms.

GLS Theory proposes: These clocks are related by simple rescaling, potentially pointing to the same underlying time concept.

📐 Four Geometric Times Explained

1. Killing Time (Static Spacetimes)

Definition:

In static spacetimes, there exists a Killing vector :

That is, the metric is invariant along .

Time Coordinate: Choose a coordinate system such that , then:

where (timelike).

Proper Time Relation:

For a stationary observer (), the proper time:

Physical Meaning:

  • describes the “time dilation factor”
  • Where the gravitational field is strong ( small), time runs slow
  • Redshift Formula:

Example: Schwarzschild Metric

, for a stationary observer:

At the horizon : (time freezes)

graph LR
    K["Killing Vector<br/>ξ^μ"] --> G["Metric Invariant<br/>£_ξ g = 0"]
    G --> V["Time Dilation<br/>V = -g_tt"]
    V --> TAU["Proper Time<br/>dτ = √V dt"]
    TAU --> RED["Gravitational Redshift<br/>ν ∝ √V"]

    style K fill:#e1f5ff
    style V fill:#fff4e1,stroke:#ff6b6b,stroke-width:3px
    style RED fill:#e1ffe1

2. ADM Lapse ( Decomposition)

ADM Decomposition:

Decompose 4-dimensional spacetime into 3-dimensional space + 1-dimensional time:

where:

  • : lapse function (ratio of coordinate time to proper time)
  • : shift vector (coordinate system drift)
  • : spatial 3-metric

Orthogonal Observer:

For an observer along the slice normal ():

Physical Meaning:

  • controls the “time flow rate”
  • : coordinate time faster than proper time
  • : coordinate time slower than proper time

ADM Equations:

Einstein’s equations can be written as constraint equations + evolution equations:

Constraints (Hamiltonian + Momentum):

Evolution:

where is the extrinsic curvature.

Relation to Killing Time:

In static spacetimes, , they are equivalent.

graph TB
    ADM["ADM Decomposition<br/>(3+1)"] --> L["lapse function<br/>N"]
    ADM --> S["shift vector<br/>N^i"]
    ADM --> H["spatial metric<br/>h_ij"]

    L --> TAU["Proper Time<br/>dτ = N dt"]
    TAU --> CON["Constraint Equations<br/>H = 0"]
    H --> EV["Evolution Equations<br/>∂_t h ~ K"]

    style ADM fill:#e1f5ff
    style L fill:#fff4e1,stroke:#ff6b6b,stroke-width:3px
    style TAU fill:#e1ffe1

3. Null Affine Parameter (Null Geodesics)

Null Geodesics:

Worldlines of light rays or massless particles, satisfying .

Geodesic Equation:

where is the tangent vector, is the affine parameter.

Why is an Affine Parameter Needed?

For null geodesics, , so we cannot parameterize with , must introduce .

Bondi Coordinates (Schwarzschild exterior):

Tortoise Coordinate:

Retarded Time:

Advanced Time:

Outgoing Null Surface:

Incoming Null Surface:

Physical Meaning:

  • are natural “boundary times”
  • In gravitational scattering, corresponds to asymptotic outgoing state time
  • Bondi mass is monotonically non-increasing along (energy radiation)

Conformal Time in FRW:

Null Geodesics:

In coordinates:

Straightening: Null geodesics appear as straight lines in conformal time.

graph LR
    NULL["Null Geodesics<br/>ds² = 0"] --> AFF["Affine Parameter<br/>λ"]
    AFF --> BONDI["Bondi Coordinates<br/>u = t - r*"]
    AFF --> CONF["Conformal Time<br/>η = ∫dt/a"]

    BONDI --> MASS["Bondi Mass<br/>M(u)↓"]
    CONF --> STRAIGHT["Straightening<br/>dη² = dχ²"]

    style NULL fill:#e1f5ff
    style AFF fill:#fff4e1,stroke:#ff6b6b,stroke-width:3px
    style BONDI fill:#ffe1e1
    style CONF fill:#e1ffe1

4. Conformal Time (FRW Universe)

FRW Metric:

where is the scale factor, is the unit 3-sphere/plane/hyperboloid metric.

Conformal Time Definition:

Integrating:

Metric Rewritten:

Physical Meaning:

  • Null geodesics are straight lines in coordinates
  • Comoving observer: (proper time = cosmic time)
  • Particle horizon: corresponds to the visible universe boundary

Redshift-Time Relation:

For photons, :

Phase Rhythm Ratio (Chapter 1):

Cosmological redshift can be viewed as a global rescaling of the time scale.

graph TB
    FRW["FRW Metric<br/>ds² = -dt² + a²dΣ²"] --> A["Scale Factor<br/>a(t)"]
    FRW --> ETA["Conformal Time<br/>dη = dt/a"]

    ETA --> STRAIGHT["Straighten Null Geodesics<br/>dη² = dχ²"]
    A --> Z["Redshift<br/>1+z = a₀/a_e"]
    Z --> PHASE["Phase Rhythm Ratio<br/>(dφ/dt)_e / (dφ/dt)₀"]

    style FRW fill:#e1f5ff
    style ETA fill:#fff4e1,stroke:#ff6b6b,stroke-width:3px
    style Z fill:#ffe1e1
    style PHASE fill:#e1ffe1

🔑 Unification of Time Equivalence Classes

Theoretical Proposition: Under appropriate conditions, the following time parameters belong to the same equivalence class:

Related to each other through affine transformations .

Proof Outline:

  1. Killing ↔ ADM: In static spacetimes, ,

  2. ADM ↔ null: The normal to ADM slices defines ,

  3. null ↔ conformal: In FRW, straightens null geodesics,

  4. conformal ↔ redshift: (with appropriate normalization)

All these transformations are affine.

graph TB
    KILLING["Killing Time<br/>dτ = √V dt"] --> ADM["ADM Time<br/>dτ = N dt"]
    ADM --> NULL["null parameter<br/>k^a∇_a k^b = 0"]
    NULL --> CONF["Conformal Time<br/>dη = dt/a"]
    CONF --> Z["Redshift<br/>1+z = a₀/a_e"]

    KILLING -.->|"N = √V"| ADM
    ADM -.->|"dλ ∝ N dt"| NULL
    NULL -.->|"straightening"| CONF
    CONF -.->|"scale factor"| Z

    ALL["Time Equivalence Class<br/>[T]"] --> KILLING
    ALL --> ADM
    ALL --> NULL
    ALL --> CONF
    ALL --> Z

    style ALL fill:#fff4e1,stroke:#ff6b6b,stroke-width:4px

📊 Connection to Unified Time Scale

Core Connection: Geometric times connect to the unified scale through the proper time-phase relation (Chapter 1):

Various Geometric Times:

  1. Killing Time:

  2. ADM Time:

  3. Conformal Time: (comoving observer)

Theoretically, they should give the same phase (along the same worldline).

Connection to Time Scale Identity:

Geometric Interpretation: is the “local time density,” integrating it gives any geometric time.

🤔 Exercises

  1. Conceptual Understanding:

    • What is the difference between Killing time and ADM time?
    • Why is a null affine parameter necessary?
    • How does conformal time straighten null geodesics?
  2. Calculation Exercises:

    • Schwarzschild metric: Calculate at
    • ADM decomposition: Prove (static case)
    • FRW universe: Calculate for matter-dominated era
  3. Physical Applications:

    • Which geometric times are involved in GPS satellite time corrections?
    • How does Bondi mass evolve with ?
    • What is the relationship between cosmological horizon and ?
  4. Advanced Thinking:

    • Can we define a global Killing time in non-static spacetimes?
    • What is the relationship between ADM energy conservation and time translation invariance?
    • What physical process corresponds to conformal time singularities?

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