Presentation on theme: "Bremsstrahlung Review – accelerated rad. Principles of brems."— Presentation transcript:
1Bremsstrahlung Review – accelerated rad. Principles of brems. Refer to Rybicki & Lightman Chapter 5 for discussion of thermal brems.Professor George F. SmootExtreme Universe Lab, SINPMoscow State University
2BREMSSTRAHLUNG RADIATION Bemsstrahlung is a German word directly describing the process: "Strahlung" means "radiation", and "Bremse" means "brake.An incoming free electron can get close to the nucleus of an atom (or other charged particle), the strong electric field of the nucleus will attract the electron, thus changing direction and speed of the electron – accelerating it.An energetic electron loses energy by emitting an X-ray photon and less energetic will emit lower energy photons. The energy of these photons will depend on the degree of interaction between nucleus and electron, i.e. the passing distance as well as the initial energy of the electron. Several subsequent interactions between one and the same electron and different nuclei are possible.X-rays originating from this process are called bremsstrahlung.Lower energy photons from this process are often called free-free emission. Free-free because the electron is free before and free after.Compare to bound-bound and free-bound interactions
4Short Review of Radiation from an Accelerated Charge – e.g. brems A charged particle accelerating in a vacuum radiates power, as described by the Larmor formula and its relativistic generalizations. Although the term "bremsstrahlung" is usually reserved for charged particles accelerating in matter, not vacuum, the formulas are similar.
5Review continued: Angular Distribution where n is a unit vector pointing from the particle towards the observer, and dW is a infinitesimal bit of solid angle.In the case where velocity is parallel to acceleration (for example, linear motion), this simplifies to
6Quantum Process Where Z is atomic number An analysis of the doubly differential cross section above shows thatelectrons whose kinetic energy is larger than the rest energy (511 keV)emit photons in forward direction while electrons with a small energy emit photons isotropically.
7For a short constant acceleration Spectrum produced in the Bremsstrahlung process.The spectrum is flat up to a cutoff frequency wcut,and falls off exponentially at higher frequencies.
8X-ray tubeIn an X-ray tube, electrons are accelerated in a vacuum by an electric field and shot into a piece of metal called the "target". X-rays are emitted as the electrons slow down (decelerate) in the metal. The output spectrum consists of a continuous spectrum of X-rays, with additional sharp peaks at certain energies (see graph on right). The continuous spectrum is due to bremsstrahlung, while the sharp peaks are characteristic X-rays associated with the atoms in the target. For this reason, bremsstrahlung in this context is also called continuous X-rays.pm is picometers
9Simple Bremsstrahlung Formula for free-free radiation Makes it easy to estimate the bremsstrahlung produced radiation field for a reasonable temperature plasma.For much hotter plasma one must take the gaunt factor in to more careful account.For reasonable temperature there is log rise
10BremsstrahlungProbability of bremsstrahlung production per atom is proportional to the square of Z of the absorberEnergy emission via bremsstrahlung varies inversely with the square of the mass of the incident particleProtons and alpha particles produce less than one-millionth the amount of bremsstrahlung radiation as electrons of the same energy
11BremsstrahlungRatio of electron energy loss by bremsstrahlung production to that lost by excitation and ionization = EZ/820E = kinetic energy of incident electron in MeVZ = atomic number of the absorberBremsstrahlung x-ray production accounts for ~1% of energy loss when 100 keV electrons collide with a tungsten (Z = 74) target in an x-ray tube
12Thermal Bremsstrahlung The emission of a single electron, with impact parameter b and velocity v.We would now like to generalize the results to a population of electrons with a certain velocity and density distribution. An astrophysically useful case is for a population with a uniform temperature T. The total emission by all particles in this population is called thermal bremsstrahlung.Consider an cloud of ionised gas with a characteristic temperature T. The velocity distribution of the particles in this cloud is given by the Maxwell distribution.In cgs units the power emitted per cubic cm isHere, gB is the frequency averaged gaunt factor for the thermal distribution of velocities, and is of order unity.
13Thermal Bremsstrahlung Power Spectrum The bremsstrahlung power spectrum rapidly decreasesfor large photon energy, and is also suppressed near theElectron plasma frequency wp.This plot is for the quantum case .
15Bethe-Heitler EqnAn analysis of the doubly differential cross section above shows that electronswhose kinetic energy is larger than the rest energy (511 keV) emit photons In forward direction while electrons with a small energy emit photons isotropically.
16Thermal Issues 2.898 x106 nm K T = max c = So what sort of temperatures and energies are involved in high energy thermal radiation? First let’s review a few equations related to electromagnetic radiation.To calculate the thermal source temperature we use Wien’s law:2.898 x106 nm KmaxT =Recall that wavelength and frequency are related via:c =where c is the speed of lightThe photon energy and momentum are related to frequency via:E = h and Momentum = h / cwhere h is Planck’s constantThis means that when a photon loses energy and momentum, its frequency n decreases.Click here to be reminded about the physical constants and units used.
17Gamma & X-rays RangesArmed with these equations, we can now see what thermal temperatures and energies are involved in high energy radiation:Gamma radiation is generally defined by photons with < nm, which corresponds E >1.24 MeV and T >108 K. Such high energy photons are created in nuclear reactions and other very high energy processes.X-rays are those photons in within the wavelength range nm < < 10 nm, with eV < E < 1.24 MeV and 106 K < T < 108 K These high energy photons are created, for example, in supernovae remnants and the solar corona, as well as in the hot gas between galaxy clusters.
18Types of Thermal Radiation You are familiar with atomic excitation and de-excitation as a means of producing photons. Thermal atomic excitation is generally via collisions, which excite atoms, and as they de-excite, they emit photons. The hotter the medium, the higher the kinetic energy of the impacts, and the higher the resulting photon energy.photon
19Thermal Bremsstrahlung As well as atomic excitation, another thermal process is bremsstrahlung radiation, which occurs when free electrons interact with ions in, for example, the hot atmospheres of stars.If a negative electron approaches a positive ion, they will be attracted to each other and the strong electric force will alter the trajectory of the electron (i.e. accelerating it), which leads to electromagnetic radiation being emitted:H+e-photonThis type of emission form is called free-free emission, or thermal bremsstrahlung - which is German for “braking radiation”.
20Energy of Thermal Bremsstrahlung The frequency range of the radiation depends on how much the electron’s trajectory is bent by the interaction with the positive ion. This depends on several things, including the relative velocities of the two bodies, which in turn depends on the temperature of the gas, which is why free-free emission is a thermal process.An example of high energy thermal bremsstrahlung is the X-ray emission from giant elliptical galaxies and hot intercluster gas.X-ray image of hot intercluster gas in Hydra A
21Bremsstrahlung Radiation Movie of the bremsstrahlung process
22BREMSSTRAHLUNG ON HEAVY NUCLEUS Movie of bremsstrahulung on a heavy nucleus with bound electrons.This is more relevant to detectors and man-generated x-rays than astro
26Characteristic X-rays The high energy electron can also cause an electron close to the nucleus in a metal atom to be knocked out from its place. This vacancy is filled by an electron further out from the nucleus. The well defined difference in binding energy, characteristic of the material, is emitted as a monoenergetic photon. When detected this X-ray photon gives rise to a characteristic X-ray line in the energy spectrum.
27Characteristic Radiation KE OF PROJECTILE ELECTRON > BINDING ENERGYORBITAL ELECTRON
31Bremsstrahlung Bremsstrahlung “Free-free Emission” “Braking” Radiation Radiation due to acceleration of charged particle by the Coulombfield of another charge.Relevant for(i) Collisions between unlike particles: changing dipole emissione-e-, p-p interactions have no net dipole moment(ii) e- - ions dominate: acc(e-) > acc(ions) because m(e-) << m(ions)recall P~m-2 ion-ion brems is negligible
32Method of Attack:(1) emission from single e-pick rest frame of ioncalculate dipole radiationcorrect for quantum effects (Gaunt factor)(2) Emission from collection of e- thermal bremsstrahlungor non-thermal bremsstrahlung(3) Relativistic bremsstrahlung (Virtual Quanta)
34Emission from Single-Speed Electrons vElectron moves past ion, assumed to be stationary.b= “impact parameter”bRZeion- Suppose the deviation of the e- path is negligible small-angle scatteringThe dipole moment is a function of time duringthe encounter.- Recall that for dipole radiationwhereis the Fourier Transform of
35After some straight-forward algebra, (R&L pp After some straight-forward algebra, (R&L pp. 156 – 157), one can derivein terms of impact parameter, b.
36Now, suppose you have a bunch of electrons, all with the same speed, v, which interact with a bunch of ions.
37Let ni = ion density (# ions/vol.) ne = electron density (# electrons / vol)The # of electrons incident on one ion isd/t# e-s /Volaround one ion, in terms of b
38So total emission/time/Vol/freq is Again, evaluating the integral is discussed in detail inR&L pWe quote the result
39Energy per volume per frequency per time due to bremsstrahlung for electrons, all with same velocity v.Gaunt factors are quantum mechanical corrections function of e- energy, frequencyGaunt factors are tabulated (more later)
40Naturally, in most situations, you never have electrons with just one velocity v.Maxwell-Boltzmann Distribution Thermal BremsstrahlungAverage the single speed expression for dW/dwdtdVover the Maxwell-Boltzmann distribution with temperature T:The result, with
41whereIn cgs units, we can write the emission coefficientergs /s /cm3 /HzFree-free emission coefficient
42Integrate over frequency: whereIn cgs:Ergs sec-1 cm-3
43The Gaunt factors - Analytical approximations exist to evaluate them - Tables exist you can look up- For most situations,so just take
45Handy table, from Tucker: Radiation Processes in Astrophysics
46Important Characteristics of Thermal Bremsstrahlung Emissivity (1) Usually optically thin. Then(2) is ~ constant with hν at low frequencies(3) falls of exponentially at
47VLA (radio region) ``image'' of Perseus A, overlayed on the X-ray image from the Chandra telescope.The central source is clearly seen, as well as radio lobeswhich loosely coincide with the two circum-nuclear``bubbles'' in the X-ray image.
48Examples: Important in hot plasmas where the gas is mostly ionized, so that bound-free emission can be neglected.T (oK)Obs. ofSolar flare107 (~ 1keV)radio flatX-ray exponentialH II region105Orion104radio-flatSco X-1108optical-flatX-ray flat/exp.Coma Cluster ICM
49Bremsstrahlung (free-free) absorption Brems emissionphotone-e-ionphotonInverse Bremss.free-free abs.e-collateralRecall the emission coefficient, jν, is related to the absorptioncoefficient αν for a thermal gas:is isotropic, soand thusin cgs:
50Important Characteristics of (1)(e.g. X-rays)Because of term,is very small unless ne is very large.in X-rays, thermal bremsstrahlung emission can betreated as optically thin(except in stellar interiors)
51(2)e.g. Radio: Rayleigh Jeans holdsAbsorption can be important, even for low nein the radio regime.
52From Bradt’s book: BB spectrum is optically thick limit of Thermal Bremss.
53HII Regions, showing free-free absorption in their radio spectra: