bb 1,2 h 3,4 he 7 li intergalactic medium interstellar medium galaxy formation inflowgal. winds,...

31
BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflow Gal. winds, stripping, mergers Cosmi c rays Smal l star s D, Li Middli ng stars Big sta rs Star formation Spallat ion 6 Li, Be, B WD NS BH SN Explosi ve r- process Winds, PN, Novae He, 7 Li, C, N D, Li, Be, B ? Nucleosynthesis Flowchart

Upload: mckayla-crace

Post on 01-Apr-2015

219 views

Category:

Documents


2 download

TRANSCRIPT

Page 1: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

BB1,2H 3,4He 7Li

Intergalactic medium

Interstellar medium

Galaxy formation inflow Gal. winds, stripping, mergers

Cosmic rays

Small stars D, Li

Middling stars

Big stars

Star formation

Spallation 6Li, Be, B

WD NS BH

SN

Explosive r-process

Winds, PN, Novae He, 7Li, C, N

D, Li, Be, B

?

Nucleosynthesis Flowchart

Page 2: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

Lecture 9: Supernova RatesStar-Formation Efficiency, Yield

How many supernovae per year for each galaxy type ?

Use power-law IMF, Salpeter slope -7/3 = -2.33

.

.Limits of validity, not well known

20 M0.1 M8 M

slope = -7/3 = -2.33

Supernova limit

Page 3: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

“Universal” IMF (Kroupa 2002)

log( M / M )

MW MC GC local

log( M / M)

M42 M35 Pleiades local ~ - 7/3 M > 1 M

- 4/3 0.1 - 1 M

- 1/3 M < 0.1 M

Page 4: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

Number of stars :

Fraction of stars with M > 8 M ( for B = -7/3 )

500 stars --> 1 supernova!

Most stars at low-mass end!

Integrating a Power-Law IMF

Page 5: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

Supernovae are rare, but each is very massive.

What fraction of the mass goes into SNe?

Most of mass is in low-mass stars.

SN Mass Fraction

Page 6: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

Median mass:

Mean mass:

.

“Typical” SN Mass

.

Page 7: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

Spiral Galaxy: SFR: ~ 8 M yr-1. 7.2% have M > 8 M .

(8 M yr-1) x 0.072 ~ 0.6 M yr-1 go into SNe

SN rate:

(fewer seen due to dust)

Irregular Galaxy: ~10x this rate during bursts (1 SN per 2 yr)!

No SNe between bursts.

.

.

SN Rates vs Galaxy Type

Page 8: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

SN Rates: Ellipticalst* = 1 Gyr e-folding time

t = 10 Gyr age= 0.95 efficiencyM0 = 1011 M total mass = initial gas massGas consumption:

Star formation:

SN rate:

3 SN per 105 yr. Negligible!

..

..

gas

stars

Page 9: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

What Star Formation Efficiency and Yields of H, He and Metals ?

X = 0.75Y = 0.25Z = 0.00

X = ?Y = ?Z = ?

MG = M0

MS = 0

MG = 0MS = M0

MG = (1-) M0

MS = M0

= ?

KABOOM!

KABOOM!

Page 10: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

Estimates for efficiency , yield in X, Y, Z

Assume:

1. Type-II SNe enrich the ISM. (Neglect: Type-I SNe, stellar winds, PNe, ....)

2. Closed Box Model: (Neglect: Infall from the IGM, outflow to the IGM)

3. SN 1987A is typical Type-II SN.

Better models include these effects.

What do we know about SN 1987A?

Page 11: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

SN 1987A23 Feb 1987 in LMC

Brightest SN since 1604!

First SN detected in neutrinos.

Visible (14 --> 4.2 mag) to naked eye, in southern sky.

Progenitor star visible: ~20 Msun blue supergiant.

3- ring structure (pre-SN wind)

UV flash reached inner ring in 80 d. Fastest ejecta reached inner ring in ~6 yr. Fast ejection velocity v~c/30~11,000 km/s. Slower (metal-enriched) ejecta asymmetric.

Page 12: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

SN 1987A23 Feb 1987 in LMC

Brightest SN since 1604!

First SN detected in neutrinos.

Visible (14 --> 4.2 mag) to naked eye, in southern sky.

Progenitor star visible:~20 Msun blue supergiant.

3- ring structure (pre-SN wind)

Shockwave reaches inner ring 2003.

20032010

Page 13: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

Use SN 1987A to calculate and yield.

SN 1987A: progenitor star mass = 20 M remnant neutron star mass = 1.6 Mmass returned to the ISM = 18.4 M

From IMF, 7.2% of MS is in stars with M > 8 M

= Fraction of MS returned to ISM:

Star Formation Efficiency = fraction of MS retained in stars:

Star Formation Efficiency

Page 14: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

SN 1987A Lightcurve

56Ni => 56 Co 6d half-life 56Co => 56 Fe 78d half-life

Powered by radioactive decay of r-process nuclei. Use to measure metal abundances in ejected gas.

Page 15: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

X, Y, Z of ejecta from SN1987A

Initial mass ~ 20 M

NS mass ~ 1.6 M

Mass ejected ~ 18.4 M

in H 9.0 M

He 7.0 M = 18.4 M

Z 2.4 M

}

Page 16: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling
Page 17: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

Q1: What changes to the particle content of the expanding Universe occur at the epochs of:

• Annihilation: – pair soup -> quark soup (109 photons/quark)

• Baryogenesis:– quarks bound (by strong force) into baryons.– UUD = proton DDU = neutron

• Nucleosynthesis:– Atomic nuclei: 75% H, 25% He, traces of Li, Be

• Recombination: – Neutral atoms form as free electrons recombine– photons fly free

Page 18: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

Q2: Given present-day density parameters M = 0.3 for matter and R = 5x10-5 for radiation, at what redshift z were the energy densities equal ?

Page 19: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

Q3 a) Evaluate the neutron/proton ratio in thermodynamic equilibrium at high and low T.

b) Evaluate the n/p ratio and Yp if mn = mp.

Page 20: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

Q4 Alien’s CMB-meter reads 5.1K and 4.9K in the fore and aft directions. Evaluate the velocity.

Are humans present on Earth at this time?

Page 21: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling
Page 22: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

Assume a Universe filled with uniform density fluid. [ OK on large scales > 100 Mpc ]

Density: Energy density:

Critical density: 3 components: 1. Radiation 2. Matter “Dark Matter” baryons 3. “Dark Energy”

Total

Cosmological Models

Only ~4% is matter as we know it!

Page 23: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

Cold Matter: ( m > 0, p << mc )

Radiation: ( m = 0 ) Hot Matter: ( m > 0, p >> mc )

Energy Density of expanding box

Page 24: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

3 Eras: radiation…matter…vacuum

Page 25: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling
Page 26: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

• Q1: Given the density parameters =0.3 for matter and =0.7 for Dark Energy, evaluate the redshift z at which the energy densities of matter and Dark Energy are equal.

= crit ~ R-3 1 + z = R0 / R= crit ~ R0

whenz

• 1+z = ( / )1/3 = ( / )1/3 = 1.326• z = 0.326

Page 27: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

• Q2: What changes to the particle content of the expanding Universe occur at the following epochs:

• Annihilation: particles and anti-particles annihilate, producing photons. Small excess of particles (~1 per 109 photons)

• Baryogenesis: free quarks confined by strong force in (colourless) groups of 3 producing neutrons (ddu) and protons (uud).

• Nucleosynthesis: protons and neutrons bind to form 2D, then 4He. Yp set by p/n ratio, as virtually all n go into 4He leaving residual p as H.

• Recombination: H and He nuclei capture free electrons. Universe now transparent to photons.

Page 28: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

• Q3: If the neutron decay time were 1 s, rather than 900s, what primordial helium abundance Yp would emerge from Big Bang Nucleosynthesis?

• n(t) = n(0) exp(- t / )• p(t) = p(0)+(n(0)-n(t))• t~300s = 900s => 1s• Yp = 2n/(p+n) => 0 since virtually all

neutrons decay.

Page 29: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

• Q4: Name and describe three effects that give rise to anisotropy in the Cosmic Microwave Background, indicating which are most important on angular scales of 10, 1 and 0.1 degrees.

• 10o Sachs-Wolf effect - photons last scattered from higher-density regions lose energy climbing out of the potential well.

• 1o Doppler effect - velocity of gas on last-scattering surface shifts photon wavelengths.

• 0.1o Sunyaev-Zeldovich effect - re-ionised gas (e.g. X-ray gas in galaxy clusters) scatters CMB photons passing thru, changing photon direction and energy.

Page 30: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling
Page 31: BB 1,2 H 3,4 He 7 Li Intergalactic medium Interstellar medium Galaxy formation inflowGal. winds, stripping, mergers Cosmic rays Small stars D, Li Middling

= fraction of M0 in gas

= fraction of M0 that has beenturned into stars

In dimensionless form

slope = -

OK, since some gas is recycled.