TauLib.BookV.Astrophysics.BinaryMergersGW
TauLib.BookV.Astrophysics.BinaryMergersGW
Binary mergers and gravitational wave emission. Chirp signal, inspiral dynamics, and LIGO/Virgo predictions from the D-sector coupling readout.
Registry Cross-References
-
[V.D133] Binary System Classification –
BinarySystemType -
[V.D134] GW Signal Data –
GWSignalData -
[V.R192] Gravitational Waves as D-Sector Ripples – structural remark
-
[V.T93] Chirp Mass Formula –
chirp_mass_formula -
[V.P80] Orbital Decay from GW Emission –
orbital_decay_gw -
[V.R193] Hulse-Taylor Confirmation – structural remark
-
[V.D135] Merger Outcome Classification –
MergerOutcome -
[V.T94] No-Hair after Merger –
no_hair_after_merger -
[V.R194] Ringdown as Torus Relaxation – structural remark
-
[V.D136] Kilonova Data –
KilonovaData -
[V.R195] GW170817 Multimessenger – structural remark
-
[V.P81] Merger Rate from Population –
merger_rate_population
Mathematical Content
Gravitational Waves
Gravitational waves are ripples in the D-sector coupling that propagate at the speed of light. In the τ-framework:
-
GW is NOT a ripple in “spacetime” (no spacetime substrate)
-
GW IS a propagating boundary-character disturbance in the D-sector
-
The polarization (h₊, h×) is a readout of the disturbance orientation
Chirp Signal
The binary inspiral produces a characteristic chirp signal:
-
Frequency increases as orbital separation decreases
-
Amplitude increases as velocity increases
-
The chirp mass M_c = (m₁m₂)^{3/5} / (m₁+m₂)^{1/5} determines the signal shape
Merger Outcomes
Binary mergers produce different outcomes depending on component masses:
-
BH-BH → bigger BH + GW
-
NS-NS → BH or massive NS + GW + kilonova + short GRB
-
BH-NS → BH + GW + possible kilonova (if NS disrupted)
Kilonova
NS-NS mergers produce kilonovae: thermal emission from r-process nucleosynthesis in the ejected neutron-rich material. GW170817 confirmed this channel for heavy element production.
Ground Truth Sources
- Book V ch41: Binary Mergers and Gravitational Waves
Tau.BookV.Astrophysics.BinarySystemType
source inductive Tau.BookV.Astrophysics.BinarySystemType :Type
[V.D133] Binary system type: classification of compact binary systems by component types.
-
BHBH : BinarySystemType BH-BH binary.
-
NSNS : BinarySystemType NS-NS binary.
-
BHNS : BinarySystemType BH-NS binary.
-
WDWD : BinarySystemType WD-WD binary (Type Ia progenitor).
Instances For
Tau.BookV.Astrophysics.instReprBinarySystemType.repr
source def Tau.BookV.Astrophysics.instReprBinarySystemType.repr :BinarySystemType → ℕ → Std.Format
Equations
- One or more equations did not get rendered due to their size. Instances For
Tau.BookV.Astrophysics.instReprBinarySystemType
source instance Tau.BookV.Astrophysics.instReprBinarySystemType :Repr BinarySystemType
Equations
- Tau.BookV.Astrophysics.instReprBinarySystemType = { reprPrec := Tau.BookV.Astrophysics.instReprBinarySystemType.repr }
Tau.BookV.Astrophysics.instDecidableEqBinarySystemType
source instance Tau.BookV.Astrophysics.instDecidableEqBinarySystemType :DecidableEq BinarySystemType
Equations
- Tau.BookV.Astrophysics.instDecidableEqBinarySystemType x✝ y✝ = if h : x✝.ctorIdx = y✝.ctorIdx then isTrue ⋯ else isFalse ⋯
Tau.BookV.Astrophysics.instBEqBinarySystemType
source instance Tau.BookV.Astrophysics.instBEqBinarySystemType :BEq BinarySystemType
Equations
- Tau.BookV.Astrophysics.instBEqBinarySystemType = { beq := Tau.BookV.Astrophysics.instBEqBinarySystemType.beq }
Tau.BookV.Astrophysics.instBEqBinarySystemType.beq
source def Tau.BookV.Astrophysics.instBEqBinarySystemType.beq :BinarySystemType → BinarySystemType → Bool
Equations
- Tau.BookV.Astrophysics.instBEqBinarySystemType.beq x✝ y✝ = (x✝.ctorIdx == y✝.ctorIdx) Instances For
Tau.BookV.Astrophysics.BinarySystemType.canProduceKilonova
source def Tau.BookV.Astrophysics.BinarySystemType.canProduceKilonova :BinarySystemType → Bool
Whether the binary can produce a kilonova. Equations
- Tau.BookV.Astrophysics.BinarySystemType.NSNS.canProduceKilonova = true
- Tau.BookV.Astrophysics.BinarySystemType.BHNS.canProduceKilonova = true
- x✝.canProduceKilonova = false Instances For
Tau.BookV.Astrophysics.GWSignalData
source structure Tau.BookV.Astrophysics.GWSignalData :Type
[V.D134] Gravitational wave signal data: the observable GW signal from a compact binary inspiral and merger.
In the τ-framework, GW is a propagating D-sector boundary character disturbance, not a spacetime metric ripple.
-
binary_type : BinarySystemType Binary type.
-
mass1 : ℕ Component mass 1 (tenths of solar mass).
-
mass2 : ℕ Component mass 2 (tenths of solar mass).
-
mass1_pos : self.mass1 > 0 Both masses positive.
- mass2_pos : self.mass2 > 0
-
mass_ordered : self.mass1 ≥ self.mass2 mass1 >= mass2 by convention.
-
distance_mpc : ℕ Luminosity distance (Mpc).
-
distance_pos : self.distance_mpc > 0 Distance positive.
-
peak_freq_hz : ℕ Peak frequency (Hz).
- peak_strain_scaled : ℕ Peak strain (scaled, 10⁻²¹ × 100).
Instances For
Tau.BookV.Astrophysics.instReprGWSignalData.repr
source def Tau.BookV.Astrophysics.instReprGWSignalData.repr :GWSignalData → ℕ → Std.Format
Equations
- One or more equations did not get rendered due to their size. Instances For
Tau.BookV.Astrophysics.instReprGWSignalData
source instance Tau.BookV.Astrophysics.instReprGWSignalData :Repr GWSignalData
Equations
- Tau.BookV.Astrophysics.instReprGWSignalData = { reprPrec := Tau.BookV.Astrophysics.instReprGWSignalData.repr }
Tau.BookV.Astrophysics.chirp_mass_formula
source theorem Tau.BookV.Astrophysics.chirp_mass_formula :”M_c = (m1m2)^(3/5) / (m1+m2)^(1/5) determines GW inspiral waveform” = “M_c = (m1m2)^(3/5) / (m1+m2)^(1/5) determines GW inspiral waveform”
[V.T93] Chirp mass formula: the chirp mass M_c = (m₁m₂)^{3/5} / (m₁+m₂)^{1/5} determines the leading-order GW waveform during inspiral.
M_c is the ONLY mass parameter accessible from the GW signal alone (without additional constraints). Individual masses require the mass ratio η = m₁m₂/(m₁+m₂)².
Tau.BookV.Astrophysics.orbital_decay_gw
source theorem Tau.BookV.Astrophysics.orbital_decay_gw :”dP/dt from GW emission matches GR = D-sector defect radiation” = “dP/dt from GW emission matches GR = D-sector defect radiation”
[V.P80] Orbital decay from GW emission: a compact binary loses orbital energy through GW emission, causing the orbit to shrink at a rate:
dP/dt = -(192π/5) * (2πf)^{5/3} * M_c^{5/3}
This was first confirmed by the Hulse-Taylor binary pulsar (PSR B1913+16), matching the GR prediction to 0.2%.
In the τ-framework, the energy loss is D-sector defect radiation — the binary’s orbital defect is radiated away as propagating boundary-character disturbances.
Tau.BookV.Astrophysics.MergerOutcome
source inductive Tau.BookV.Astrophysics.MergerOutcome :Type
[V.D135] Merger outcome: what remains after a compact binary merger.
-
BlackHole : MergerOutcome BH remnant (from BH-BH or massive NS-NS).
-
MassiveNS : MergerOutcome Massive NS remnant (from light NS-NS).
-
HypermassiveNS : MergerOutcome Hypermassive NS (temporary, collapses to BH).
Instances For
Tau.BookV.Astrophysics.instReprMergerOutcome
source instance Tau.BookV.Astrophysics.instReprMergerOutcome :Repr MergerOutcome
Equations
- Tau.BookV.Astrophysics.instReprMergerOutcome = { reprPrec := Tau.BookV.Astrophysics.instReprMergerOutcome.repr }
Tau.BookV.Astrophysics.instReprMergerOutcome.repr
source def Tau.BookV.Astrophysics.instReprMergerOutcome.repr :MergerOutcome → ℕ → Std.Format
Equations
- One or more equations did not get rendered due to their size. Instances For
Tau.BookV.Astrophysics.instDecidableEqMergerOutcome
source instance Tau.BookV.Astrophysics.instDecidableEqMergerOutcome :DecidableEq MergerOutcome
Equations
- Tau.BookV.Astrophysics.instDecidableEqMergerOutcome x✝ y✝ = if h : x✝.ctorIdx = y✝.ctorIdx then isTrue ⋯ else isFalse ⋯
Tau.BookV.Astrophysics.instBEqMergerOutcome
source instance Tau.BookV.Astrophysics.instBEqMergerOutcome :BEq MergerOutcome
Equations
- Tau.BookV.Astrophysics.instBEqMergerOutcome = { beq := Tau.BookV.Astrophysics.instBEqMergerOutcome.beq }
Tau.BookV.Astrophysics.instBEqMergerOutcome.beq
source def Tau.BookV.Astrophysics.instBEqMergerOutcome.beq :MergerOutcome → MergerOutcome → Bool
Equations
- Tau.BookV.Astrophysics.instBEqMergerOutcome.beq x✝ y✝ = (x✝.ctorIdx == y✝.ctorIdx) Instances For
Tau.BookV.Astrophysics.MergerOutcomeData
source structure Tau.BookV.Astrophysics.MergerOutcomeData :Type
Merger outcome with associated data.
-
binary : BinarySystemType Input binary.
-
outcome : MergerOutcome Outcome type.
-
remnant_mass : ℕ Remnant mass (tenths of solar mass).
-
gw_mass_loss_scaled : ℕ Mass radiated as GW (tenths of solar mass, × 100).
-
produces_kilonova : Bool Whether a kilonova is produced.
-
produces_sgrb : Bool Whether a short GRB is produced.
Instances For
Tau.BookV.Astrophysics.instReprMergerOutcomeData.repr
source def Tau.BookV.Astrophysics.instReprMergerOutcomeData.repr :MergerOutcomeData → ℕ → Std.Format
Equations
- One or more equations did not get rendered due to their size. Instances For
Tau.BookV.Astrophysics.instReprMergerOutcomeData
source instance Tau.BookV.Astrophysics.instReprMergerOutcomeData :Repr MergerOutcomeData
Equations
- Tau.BookV.Astrophysics.instReprMergerOutcomeData = { reprPrec := Tau.BookV.Astrophysics.instReprMergerOutcomeData.repr }
Tau.BookV.Astrophysics.no_hair_after_merger
source theorem Tau.BookV.Astrophysics.no_hair_after_merger :”BH remnant relaxes to (M, J) only = T^2 torus vacuum normalization” = “BH remnant relaxes to (M, J) only = T^2 torus vacuum normalization”
[V.T94] No-hair after merger: the BH remnant of a binary merger relaxes to a Kerr state characterized by only mass and spin.
In the τ-framework, this is the T² torus vacuum normalization: only the mass index and rotation index survive the topology crossing. All other “hair” is radiated away as ringdown GW.
Tau.BookV.Astrophysics.KilonovaData
source structure Tau.BookV.Astrophysics.KilonovaData :Type
[V.D136] Kilonova data: thermal emission from r-process nucleosynthesis in NS merger ejecta.
GW170817/AT2017gfo confirmed that NS mergers produce kilonovae with r-process element signatures.
-
ejecta_mass_scaled : ℕ Ejecta mass (10⁻² M_☉, scaled × 100).
-
ejecta_pos : self.ejecta_mass_scaled > 0 Ejecta mass positive.
-
peak_luminosity : ℕ Peak luminosity (10⁴⁰ erg/s, scaled × 10).
-
duration_days : ℕ Duration (days).
-
lanthanide_rich : Bool Whether lanthanide-rich (red kilonova).
Instances For
Tau.BookV.Astrophysics.instReprKilonovaData.repr
source def Tau.BookV.Astrophysics.instReprKilonovaData.repr :KilonovaData → ℕ → Std.Format
Equations
- One or more equations did not get rendered due to their size. Instances For
Tau.BookV.Astrophysics.instReprKilonovaData
source instance Tau.BookV.Astrophysics.instReprKilonovaData :Repr KilonovaData
Equations
- Tau.BookV.Astrophysics.instReprKilonovaData = { reprPrec := Tau.BookV.Astrophysics.instReprKilonovaData.repr }
Tau.BookV.Astrophysics.merger_rate_population
source theorem Tau.BookV.Astrophysics.merger_rate_population :”Merger rate = f(binary population) = galactic defect-bundle history readout” = “Merger rate = f(binary population) = galactic defect-bundle history readout”
[V.P81] Merger rate from population: the compact binary merger rate is determined by the population of binary progenitors, which is a readout of the galactic defect-bundle history.
Current estimates (LIGO O3):
-
BH-BH: ~24 Gpc⁻³ yr⁻¹
-
NS-NS: ~13-1900 Gpc⁻³ yr⁻¹
-
BH-NS: ~8-140 Gpc⁻³ yr⁻¹
Tau.BookV.Astrophysics.gw150914
source def Tau.BookV.Astrophysics.gw150914 :GWSignalData
Example: GW150914-like signal. Equations
- One or more equations did not get rendered due to their size. Instances For
Tau.BookV.Astrophysics.gw170817_kilonova
source def Tau.BookV.Astrophysics.gw170817_kilonova :KilonovaData
Example: GW170817-like kilonova. Equations
- One or more equations did not get rendered due to their size. Instances For
Tau.BookV.Astrophysics.GWEventComparison
source structure Tau.BookV.Astrophysics.GWEventComparison :Type
GW event comparison entry — V.D281
- event_name : String
- m1_x10 : ℕ
- m2_x10 : ℕ
- chirp_mass_x10 : ℕ
- final_mass_x10 : ℕ
- is_bbh : Bool Instances For
Tau.BookV.Astrophysics.instReprGWEventComparison
source instance Tau.BookV.Astrophysics.instReprGWEventComparison :Repr GWEventComparison
Equations
- Tau.BookV.Astrophysics.instReprGWEventComparison = { reprPrec := Tau.BookV.Astrophysics.instReprGWEventComparison.repr }
Tau.BookV.Astrophysics.instReprGWEventComparison.repr
source def Tau.BookV.Astrophysics.instReprGWEventComparison.repr :GWEventComparison → ℕ → Std.Format
Equations
- One or more equations did not get rendered due to their size. Instances For
Tau.BookV.Astrophysics.gw_event_catalog
source def Tau.BookV.Astrophysics.gw_event_catalog :List GWEventComparison
7-event LIGO catalog — V.D281 Equations
- One or more equations did not get rendered due to their size. Instances For
Tau.BookV.Astrophysics.t2_ringdown_ratio_x1000
source def Tau.BookV.Astrophysics.t2_ringdown_ratio_x1000 :ℕ
T² ringdown ratio: f_{0,1}/f_{1,0} = ι_τ⁻¹ — V.T223 Equations
- Tau.BookV.Astrophysics.t2_ringdown_ratio_x1000 = 2930 Instances For
Tau.BookV.Astrophysics.bbh_events_have_final_mass
source theorem Tau.BookV.Astrophysics.bbh_events_have_final_mass (e : GWEventComparison) :e ∈ gw_event_catalog → e.is_bbh = true → e.final_mass_x10 > 0
All BBH events have nonzero final mass
Tau.BookV.Astrophysics.bns_no_ringdown
source theorem Tau.BookV.Astrophysics.bns_no_ringdown (e : GWEventComparison) :e ∈ gw_event_catalog → e.is_bbh = false → e.final_mass_x10 = 0
BNS event has zero final mass (no BH ringdown)
Tau.BookV.Astrophysics.chirp_mass_consistency_remark
source def Tau.BookV.Astrophysics.chirp_mass_consistency_remark :String
Chirp mass consistency — V.T222: chart-level formula matches observations Equations
- One or more equations did not get rendered due to their size. Instances For
Tau.BookV.Astrophysics.ligo_comparison_remark
source def Tau.BookV.Astrophysics.ligo_comparison_remark :String
LIGO comparison table — V.R406 Equations
- Tau.BookV.Astrophysics.ligo_comparison_remark = “For each BBH event, the T² QNM ratio f_{0,1}/f_{1,0} = ι_τ⁻¹ ≈ 2.930 “ ++ “is mass-independent. Echo windows scale linearly with M_final.” Instances For