Single shot emittance measurement using Optical Transition Radiation

# Single shot emittance measurement using Optical Transition Radiation

We describe a method that uses Optical Transition Radiation (OTR) screens to measure in a single shot the emittance of an electron beam with an energy greater than 100 MeV. Our setup consists of 4 OTR screens located near a beam waist. A fit of the 4 profiles allows the reconstruction of the Twiss parameters and hence a calculation of the beam emittance. This layout has been simulated using Mathematica to study its sensitivity to errors and using Geant4 to include effects due to the scattering of the electrons in the screens.

Some assumptions made in this document are conservative to allow for unexpected experimental issues.

## 1 Emittance measurement using several screens

### 1.1 Proposed experiments

The measurement of a beam emittance by using several screens one after the other in a linac is a well know technique. We propose to adapt this technique to single shot emittance measurements by using the screens simultaneously. This requires the use of very thin screens. In our simulations we have used 3 screens located 0.5m apart from each other followed by a 4th screen located 1m beyond the 3rd screen.

### 1.2 Beam propagation in a drift space

In a drift space the beam () size evolves as [CAS94]:

 σ(s)=√ϵ(β0−2α0s+γ0s2) (1)

where is the position in the drift space, , and are the Twiss parameters at and is the beam emittance.

When is a symmetry point (waist), this can be rewritten as

 σ(s)=√ϵβ0+ϵβ0s2 (2)

By measuring with an OTR screen at 3 (or more) locations around a waist it is thus possible to make a parabolic fit giving the Twiss parameters of the beam as well as and .

### 1.3 Beam expansion condition

In such drift space the beam divergence is (with a different sign on either side of the waist)

 σ′=±√ϵβ=±ϵσ0 (3)

with the beam size at the waist.

The beam size at a given distance from the waist will be related to the beam size at the waist by the following relation:

 σ(s)σ0 = √ϵβ0+ϵβ0s2√ϵβ0 (4) = √1+s2β20

Using , this becomes:

 σ(s)σ0 = √1+ϵ2s2σ40 (5)

Hence for a 1 mm.mrad beam with a 1 mm spot size, the beam will have increased by 10% beam at m and by 20% at m. For the same beam with a 5mm spot size, these distances are multiplied by 25 and become m and m. Figure 2 gives the beam enveloppes for various emittances and beam waist sizes.

### 1.4 Effect of the scattering in the screens on the beam expansion

An electron traversing nuclear matter will be Coulomb scattered. Most of these scattering will be at very small angle but will add up as the electron progresses through the matter. The phenomena is described in details in [PDG].

For a bunch of electron, the scattering experienced after traversing a layer of thickness can be approximated by a Gaussian of width[Lynch:1990sq]:

 θ0=13.6 MeVβcp√xX0[1+0.038ln(xX0)] (6)

where is the velocity of the electrons, p their momentum and a quantity called the radiation length and which expresses how high energy electrons loose their energy in a given material1.

To make it easier to estimate the scattering as a function of the momentum this equation can be rewritten as

 pθ0=13.6 MeVβc√xX0[1+0.038ln(xX0)] (7)

Table 1 shows that the electrons will travel only a small fraction of a radiation length () in each type of screen considered. A scattering factor of the order of a hundred MeV.mrad means that a beam with an energy of a hundreds MeV will be scattered by about one milliradian. Among the different screens considered, Mylar and Kapton (Polyimide film) introduce the lower scattering and thinner films seems available.

When the beam scatters on the screens an additional scattering term is required and equation 1 is approximately modified as follow:

 σ(s)=√ϵ(β0−2α0s+γ0s2)+N(s)screens∑i=1(s−si)θ2i (8)

where is the number of screens located upstream from the position at which the measurement is performed, their position and the scattering they induce.

Assuming that all screens are made of the same material with a scattering coefficient , the scattering induced by the first screen will dominate:

 N(s)screens∑i=1(s−si)θi≃(s−s1)θ0 (9)

A measurement of the beam size dominated by the term will provide information on the scattering but not on the emittance of the beam. Hence the screens, their position and the beam optics must be chosen so that in all measurements the scattering can be neglected.

This requires:

 ϵσ0s>Nscreensθ0(s−s1) (10)

where is the total number of screens used.

Assuming that the first screen is close from the waist and hence , this can be rewritten as:

 ϵσ0>>Nscreensθ0 (11) σ0<<ϵNscreensθ0 (12)

Equation 12 can be rewritten as

 σ0<

where is the normalised emittance, the Lorentz transformation factor and c the speed of light.

This shows that the requirement on as a function of the normalised emittance and of is independent of the beam energy (but the ease of achieving a given may be different).

At 500 MeV a m polyimide film screen will induce a scattering mrad. With an emittance mm.mrad, equation 12 requires mm. The limit value of as given by equation 12 assuming for various screen materials is given in table 1.

When the spot size is chosen so that equation 12 is satisfied the scattering can be neglected, it is the case with thin Mylar or kapton screens .

## 2 Simulations

### 2.1 Mathematica

Simple simulations of such measurement have been done using Mathematica. In these simulations 4 screens were positioned at , , and . The propagation of a beam with a given emittance and beta function was then calculated and the size of the beam at each screen was estimated with some noise added. To take into account the limited pixel size the measured beam size was rounded to the size of the pixels.

If the beam optics or the beam energy is not well understood the beam waist may not be positioned exactly where it is expected to be, this was included in our simulations.

Equation 2 was fitted to the beam sizes found and from this fit the value of the emittance was deducted. With the beam sizes used it is assumed that the effect of the scattering can be neglected as the natural beam divergence is much bigger than the divergence induced (equation 12).

Figure 3 shows a few example of such fits.

Figure 4 shows the difference between the deducted emittance and the real emittance for several simulation runs.

Figure 5 shows the difference between the deducted emittance and the real emittance for several simulation runs where the waist position has been varied. These simulations show when the actual waist is far from the performances of the fit are significantly degraded (this is also visible on figure 3c).

### 2.2 Geant4

To better simulate the effect of the scattering in the screens we have used the Geant4 Toolkit [Agostinelli:2002hh].

We have used the Geant Low Energy Physics processes [Apostolakis:1999bp]. These processes are valid from 250eV to 100GeV [Chauvie:2001fh] and so completely cover the range of energies we are interested in.

In our simulations the electrons were fired from a source on screens placed 0.5m, 1.0m, 1.5m and 2.5m after the source. The initial direction of the electrons was so that they formed a 2mm waist 1m after the source. A 10-thick Mylar window was located 1mm after the electron source.

The position at which the electrons traversed each screen as well as intermediate detectors was recorded. For each simulation more approximately 10 000 electrons were fired.

#### Effect of the air pressure

Our first study focused on the effect of scattering in the air contained in the vacuum vessel. The propagation of the beam in the absence of screen in an atmosphere filled with air at different pressures was studied. Figure 6 shows that for pressure higher than 10 mbar the scattering over 2m is significant and thus can not be neglected.

#### Emittance measurement

To study the effect of the scattering in the screens several simulations were done using different materials and thicknesses for the screens. Some of the simulations for beams of 200 MeV are shown in figure 7 and for 500 MeV beam in figure 8. As one can see on the figures the use of thin Mylar screens leads to better results than with Aluminium. Furthermore thin Mylar films are easier to handle.

The previous studies assumed that the beam waist was located on the second screen. Figure 9 shows that the emittance can still be reconstructed with a reasonable accuracy when the waist is elsewhere (between the screens).

Commercially we found some -thick Mylar coated with a 10nm layer of Aluminium. Neglecting the scattering in the aluminium, the emittance fit can be seen on figure 10.

## 3 Conclusions

We have studied how 4 screens introduced simultaneously in a beam line could be used to fit the Twiss parameters of an electron beam in a single shot measurement. We have shown that by using -thick Mylar screen such fit would lead to a measurement of the beam transverse emittance correct within 15% for a 500 MeV beam and within 30% for a 200 MeV beam.

## References

### Footnotes

1. The radiation length is the mean distance over which a high-energy electron looses all but 1/ of its energy by Bremstrahlung[PDG].
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