Asymmetric 2‐bounce monochromator for quasi‐fixed offset
In many monochromatic x‐ray applications, it is important to maintain a constant direction of the monochromatized beam, preferably parallel to the direction of the original beam. For the most exacting applications, independent‐crystal two‐bounce monochromators can be used. These however, are costly...
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Veröffentlicht in: | Review of Scientific Instruments 1996-09, Vol.67 (9), p.3352-3352 |
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description | In many monochromatic x‐ray applications, it is important to maintain a constant direction of the monochromatized beam, preferably parallel to the direction of the original beam. For the most exacting applications, independent‐crystal two‐bounce monochromators can be used. These however, are costly and cumbersome. Therefore, in less demanding situations or when space is at premium, two‐bounce channel‐cut monochromators are commonly used. Unfortunately, while the direction of the beam emerging from a channel‐cut monochromator is fixed, the beam offset varies with the angle of incidence, i.e., with the energy of the monochromatic beam. This complicates experiments in which it is important to maintain the beam on a fixed spot of the sample. We show, however, that the variation of beam offset in channel‐cut monochromators can be greatly reduced by introducing a small amount of asymmetry into the cut. The exact amount of asymmetry (typically a few degrees) depends, of course, on the crystal and the energy range. We will present a full mathematical analysis and a design of a working monochromator based on this scheme. |
doi_str_mv | 10.1063/1.1147259 |
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For the most exacting applications, independent‐crystal two‐bounce monochromators can be used. These however, are costly and cumbersome. Therefore, in less demanding situations or when space is at premium, two‐bounce channel‐cut monochromators are commonly used. Unfortunately, while the direction of the beam emerging from a channel‐cut monochromator is fixed, the beam offset varies with the angle of incidence, i.e., with the energy of the monochromatic beam. This complicates experiments in which it is important to maintain the beam on a fixed spot of the sample. We show, however, that the variation of beam offset in channel‐cut monochromators can be greatly reduced by introducing a small amount of asymmetry into the cut. The exact amount of asymmetry (typically a few degrees) depends, of course, on the crystal and the energy range. 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For the most exacting applications, independent‐crystal two‐bounce monochromators can be used. These however, are costly and cumbersome. Therefore, in less demanding situations or when space is at premium, two‐bounce channel‐cut monochromators are commonly used. Unfortunately, while the direction of the beam emerging from a channel‐cut monochromator is fixed, the beam offset varies with the angle of incidence, i.e., with the energy of the monochromatic beam. This complicates experiments in which it is important to maintain the beam on a fixed spot of the sample. We show, however, that the variation of beam offset in channel‐cut monochromators can be greatly reduced by introducing a small amount of asymmetry into the cut. The exact amount of asymmetry (typically a few degrees) depends, of course, on the crystal and the energy range. We will present a full mathematical analysis and a design of a working monochromator based on this scheme.</description><subject>ASYMMETRY</subject><subject>DESIGN</subject><subject>INSTRUMENTATION, INCLUDING NUCLEAR AND PARTICLE DETECTORS</subject><subject>MONOCHROMATORS</subject><subject>PARTICLE ACCELERATORS</subject><subject>SYNCHROTRON RADIATION SOURCES</subject><subject>X-RAY EQUIPMENT</subject><issn>0034-6748</issn><issn>1089-7623</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1996</creationdate><recordtype>article</recordtype><recordid>eNp90M1KAzEUBeAgCtbqwjcYlwpTcyeZZAbclOIfFNzoOqSZXBpxJjVJxe58BJ_RJ3HKFF0IXjjczcdZHEJOgU6ACnYJEwAui7LeIyOgVZ1LUbB9MqKU8VxIXh2SoxifaX8lwIhcTeOmbW0KzmTF18fnwq87Y7PWd94sg2918iHDPq9rHV0P0L3bJvOI0aZjcoD6JdqT3R-Tp5vrx9ldPn-4vZ9N57kpOE15g7ygmlPgdVUyJhCM5cjAVCgLzWgtjBSWsgIsgOAoayaY1BLrhkkUCzYmZ0Ovj8mpaFyyZml811mTFGdclqI354MxwccYLKpVcK0OGwVUbadRoHbT9PZisNsqnZzvfvCbD79QrRr8D_9t_gbaBHKQ</recordid><startdate>199609</startdate><enddate>199609</enddate><creator>Schildkamp, W.</creator><creator>Meron, M.</creator><scope>AAYXX</scope><scope>CITATION</scope><scope>OTOTI</scope></search><sort><creationdate>199609</creationdate><title>Asymmetric 2‐bounce monochromator for quasi‐fixed offset</title><author>Schildkamp, W. ; Meron, M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c240t-df420a4014985336f1ce4f31c8f72a3096c76e0321e1164f793637a7f9d37f6b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1996</creationdate><topic>ASYMMETRY</topic><topic>DESIGN</topic><topic>INSTRUMENTATION, INCLUDING NUCLEAR AND PARTICLE DETECTORS</topic><topic>MONOCHROMATORS</topic><topic>PARTICLE ACCELERATORS</topic><topic>SYNCHROTRON RADIATION SOURCES</topic><topic>X-RAY EQUIPMENT</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Schildkamp, W.</creatorcontrib><creatorcontrib>Meron, M.</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Review of Scientific Instruments</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Schildkamp, W.</au><au>Meron, M.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Asymmetric 2‐bounce monochromator for quasi‐fixed offset</atitle><jtitle>Review of Scientific Instruments</jtitle><date>1996-09</date><risdate>1996</risdate><volume>67</volume><issue>9</issue><spage>3352</spage><epage>3352</epage><pages>3352-3352</pages><issn>0034-6748</issn><eissn>1089-7623</eissn><coden>RSINAK</coden><abstract>In many monochromatic x‐ray applications, it is important to maintain a constant direction of the monochromatized beam, preferably parallel to the direction of the original beam. For the most exacting applications, independent‐crystal two‐bounce monochromators can be used. These however, are costly and cumbersome. Therefore, in less demanding situations or when space is at premium, two‐bounce channel‐cut monochromators are commonly used. Unfortunately, while the direction of the beam emerging from a channel‐cut monochromator is fixed, the beam offset varies with the angle of incidence, i.e., with the energy of the monochromatic beam. This complicates experiments in which it is important to maintain the beam on a fixed spot of the sample. We show, however, that the variation of beam offset in channel‐cut monochromators can be greatly reduced by introducing a small amount of asymmetry into the cut. The exact amount of asymmetry (typically a few degrees) depends, of course, on the crystal and the energy range. We will present a full mathematical analysis and a design of a working monochromator based on this scheme.</abstract><cop>United States</cop><doi>10.1063/1.1147259</doi><tpages>1</tpages></addata></record> |
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subjects | ASYMMETRY DESIGN INSTRUMENTATION, INCLUDING NUCLEAR AND PARTICLE DETECTORS MONOCHROMATORS PARTICLE ACCELERATORS SYNCHROTRON RADIATION SOURCES X-RAY EQUIPMENT |
title | Asymmetric 2‐bounce monochromator for quasi‐fixed offset |
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