Indus-1 Beamlines

PASS Beamline


Introduction

The PASS beamline will be used to measure the absorption spectra of solid samples of low Z (C, N, O, Ti, V) material both in thin film as well as bulk form. The beamline is indigenous developed and cover the energy range of 55eV to 840 eV. The absorption spectra both in XANES (X-ray Absorption Near Edge Structure) and EXAFS (Extended X-ray Absorption Fine Structure) mode of low Z-materials can be measured. Currently we are using total electron yield (TEY) mode of XAFS. The Schematic of the PASS beamline is given in Fig.1.

The complete beamline is maintained in ultra-high vacuum (UHV) environment. The major components of the beamline (Fig. 2, 3 and 4) include a SX-700 type plane grating monochromator (PGM) based having plane mirror and plane grating. The energy range of the beamline is covered by rotation of grating and simultaneously rotation as well as translation of the plane mirror using high precision motorized drives. The pivot of the grating is lying on the surface of grating and pivot of the mirror is lying outside the mirror surface. The next major component is ellipsoidal mirror to focus the beam at the slit in both meridional and sagittal plane.

The experimental station of the beamline consists of 4-axis motion sample manipulator, sample holder facilitated with sample current measurement (Is), Ni mesh for initial current measurement (I0),

The sample current Isis given by
Is = I0 exp(-μt)


Where μ absorption coefficient of material, t is the thickness upto the layer from which the electrons are coming out.
Fig.1: Schematic of the PASS beamline
Fig.1: Schematic of the PASS beamline

Beamline Specifications:

Source Bending magnet BM02
Length of the beamline 17.5 mtrs from the tangent point
Energy Range 55 eV – 840 eV
Acceptance of the beam 2.6 mrad (H) X 0.25 mrad (V)
Monochromator SX-700 type PGM
No. of Grating 1 (groove density : 1198 l/mm)
Energy Resolution (ΔE/E) ~10-3
Flux (at the sample) 109 ph/s


Fig.2: 3D view of PASS beamline
Fig.2: 3D view of PASS beamline


Fig.3: PASS beamline
Fig.3: PASS beamline


Fig.4: Major components of PASS beamline
Fig.4: Major components of PASS beamline


Fig.5: Inside view of in-house developed Plane Grating Monochromator
Fig.5: Inside view of in-house developed Plane Grating Monochromator


Fig. 6:  Experimental station of PASS beamline
Fig. 6: Experimental station of PASS beamline

Result

Fig.7: Oxygen K-edge of ZnO  where  a, b, c and d are pre-edge peaks due to different hybridized levels
Fig.7: Oxygen K-edge of ZnO where a, b, c and d are pre-edge peaks due to different hybridized levels


Fig.8: Nitrogen K-edge of Magnesium Pthalocynine (MgPc) film
Fig.8: Nitrogen K-edge of Magnesium Pthalocynine (MgPc) film


Fig.9: Carbon K-edge of MgPc peaks a and b corresponds to 1s- 𝜋* and 1s- 𝜎*transition.
Fig.9: Carbon K-edge of MgPc peaks a and b corresponds to 1s- 𝜋* and 1s- 𝜎*transition.

Present Status

The trial experiments on several samples have been performed

Contact Number: 91-731- 244- 8114/2118

In-charge:

Dr. R. K. Sharma      Email: sharmark@rrcat.gov.in

Other contributers:

Dr. Jagannath ssai@barc.gov.in Technical Physics Division Bhabha Atomic Research Centre, Mumbai – 400 085.
Shri Jaspreet Singh jaspreet@rrcat.gov.in
Shri Uday Sule usule@rrcat.gov.in
Shri Pradeep R jpradeepr@barc.gov.in


Last Updated on: September 2020
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