Machine:Insertion Devices

Phase 1 Beamlines

As of now there is only a preliminary list of insertion devices (IDs) which are being considered for installation in the storage ring at phase 1. IDs for phase 2 are not yet defined, although for the purpose of beam dynamics calculations we consider more than doubling phase 1 IDs.Table 1 lists all insertion devices

Table 1: Sirius beamline IDs for Phase 1 Beamline Commissioning ID Final ID Straight Section Carnaúba APU22 Delta21 06SB (low β) Cateretê APU22 Delta21 07SP (low β) Ema APU22 APU19 08SB (low β) Manacá APU22 APU20 09SA (high β) Sabiá Delta52 10SB (low β) Ipê APU58 Delta52 11SP (low β) PGM++ Delta52 12SB (low β)
Insertion device Delta21 Name Delta21 Unit Type Delta Period length (λ) 21 mm Number of periods (Np) 114 Length (L) 240 cm Gap (G) 7.00 mm Maximum Power @ 500 mA 8.6 kW Horizontal Vertical Maximum Field 0.00 1.12 T Maximum K 0.0 2.2	Insertion device APU19 Name APU19 Unit Type APU Period length (λ) 19 mm Number of periods (Np) 126 Length (L) 240 cm Gap (G) 5.00 mm Maximum Power @ 500 mA 11.2 kW Horizontal Vertical Maximum Field 0.00 1.28 T Maximum K 0.0 2.3
Insertion device Delta52 Name Delta52 Unit Type Delta Period length (λ) 52.5 mm Number of periods (Np) 69 Length (L) 360 cm Gap (G) 13.85 mm Maximum Power @ 500 mA 14.6 kW Horizontal Vertical Maximum Field 0.00 1.19 T Maximum K 0.0 5.85	Insertion device APU20 Name APU20 Unit Type APU Period length (λ) 20 mm Number of periods (Np) 120 Length (L) 240 cm Gap (G) 6.20 mm Maximum Power @ 500 mA 7.8 kW Horizontal Vertical Maximum Field 0.00 1.07 T Maximum K 0.0 2.0

Each of these IDs has impact over the properties of the beam, be it on the long term dynamic stability or on the equilibrium parameters. Figure 1 shows the effect of IDs over emittance and beam energy spread, in particular.

Figure 1: Effect of insertion devices on the Sirius natural emittance and energy spread for Phase-1 IDs and hypothetical Phase-2 IDs.

Commissioning Undulators

Five planar unduladors (APUs) were purchased from Kyma to be installed in the storage ring for the commisioning phase of some beamlines. Table 2 shows the relation of the IDs used in each beamline and their main parameters

Table 2: Sirius beamline IDs for Commissioning Beamline ID name ID Type Straight Section ID code Carnaúba SI-06SB:ID-APU22 APU22 06SB (low β) 1991c Cateretê SI-07SP:ID-APU22 APU22 07SP (low β) 1991a Ema SI-08SB:ID-APU22 APU22 08SB (low β) 1991d Manacá SI-09SA:ID-APU22 APU22 09SA (high β) 1991b Ipê SI-11SP:ID-APU58 APU58 11SP (low β) 1995
Insertion device APU22 Name APU22 Unit Type APU Period length (λ) 22 mm Number of periods (Np) 51 Length (L) 120 cm Gap (G) 8 mm Maximum Power @ 500 mA 1.6 kW Horizontal Vertical Maximum Field 0.00 0.7 T Maximum K 0.0 1.4	Insertion device APU58 Name APU58 Unit Type APU Period length (λ) 58 mm Number of periods (Np) 18 Length (L) 120 cm Gap (G) 15.8 mm Maximum Power @ 500 mA 3.1 kW Horizontal Vertical Maximum Field 0.00 0.95 T Maximum K 0.0 5.2

The analysis of the magnetic and beam measurements for these undulators are shown below:

1991a (SI-07SP:ID-APU22 for the Cateretê beamline)

Figure 2: Excitation curve of undulator 1991a for x=0.0mm and y=+0.0mm
Figure 3:	Figure 4:

1991b (SI-09SA:ID-APU22 for the Manacá beamline)

Figure 5: Excitation curve of undulator 1991b for x=0.0mm and y=+0.0mm
Figure 6: Field Amplitudes for undulator 1991b as function of phases for several x for y=-01.0mm	Figure 7: Field Amplitudes for undulator 1991b as function of phases for several x for y=00.0mm	Figure 8: Field Amplitudes for undulator 1991b as function of phases for several x for y=+01.0mm
Figure 9: Field Integrals for undulator 1991b measured with the coil system as function of x for several phases for y=-01.0mm	Figure 10: Field Integrals for undulator 1991b measured with the coil system as function of x for several phases for y=00.0mm	Figure 11: Field Integrals for undulator 1991b measured with the coil system as function of x for several phases for y=+01.0mm

1991c (SI-06SB:ID-APU22 for the Carnaúba beamline)

Figure 12: Excitation curve of undulator 1991c for x=0.0mm and y=+1.0mm
Figure 13: Field Amplitudes for undulator 1991c as function of phases for several x for y=-01.0mm	Figure 14: Field Amplitudes for undulator 1991c as function of phases for several x for y=00.0mm	Figure 15: Field Amplitudes for undulator 1991c as function of phases for several x for y=+01.0mm
Figure 16: Field Integrals for undulator 1991c measured with the coil system as function of x for several phases for y=-01.0mm	Figure 17: Field Integrals for undulator 1991c measured with the coil system as function of x for several phases for y=00.0mm	Figure 18: Field Integrals for undulator 1991c measured with the coil system as function of x for several phases for y=+01.0mm

1991d (SI-08SB:ID-APU22 for the Ema beamline)

Figure 19: Excitation curve of undulator 1991d for x=0.0mm and y=+1.0mm
Figure 20: Field Amplitudes for undulator 1991d as function of phases for several x for y=-01.0mm	Figure 21: Field Amplitudes for undulator 1991d as function of phases for several x for y=00.0mm	Figure 22: Field Amplitudes for undulator 1991d as function of phases for several x for y=+01.0mm
Figure 23: Field Integrals for undulator 1991d measured with the coil system as function of x for several phases for y=-01.0mm	Figure 24: Field Integrals for undulator 1991d measured with the coil system as function of x for several phases for y=00.0mm	Figure 25: Field Integrals for undulator 1991d measured with the coil system as function of x for several phases for y=+01.0mm
Figure 26: Field Integrals for undulator 1991d measured with the hall system as function of x for several phases for y=-01.0mm	Figure 27: Field Integrals for undulator 1991d measured with the hall system as function of x for several phases for y=00.0mm	Figure 28: Field Integrals for undulator 1991d measured with the hall system as function of x for several phases for y=+01.0mm

1995 (SI-11SP:ID-APU58 for the Ipê beamline)

Figure 29: Excitation curve of undulator 1995 for x=0.0mm and y=+1.0mm
Figure 30: Field Amplitudes for undulator 1995 as function of phases for several x for y=-01.0mm	Figure 31: Field Amplitudes for undulator 1995 as function of phases for several x for y=00.0mm	Figure 32: Field Amplitudes for undulator 1995 as function of phases for several x for y=+01.0mm
Figure 33: Field Integrals for undulator 1995 measured with the coil system as function of x for several phases for y=-01.0mm	Figure 34: Field Integrals for undulator 1995 measured with the coil system as function of x for several phases for y=00.0mm	Figure 35: Field Integrals for undulator 1995 measured with the coil system as function of x for several phases for y=+01.0mm
Figure 36: Field Integrals for undulator 1995 measured with the hall system as function of x for several phases for y=-01.0mm	Figure 37: Field Integrals for undulator 1995 measured with the hall system as function of x for several phases for y=00.0mm	Figure 38: Field Integrals for undulator 1995 measured with the hall system as function of x for several phases for y=+01.0mm