DESIGN CONSIDERATION OF ONE METER LONG UNDULATOR* Geetanjali Sharma, Roma Khullar, Mona Gehlot, G Mishra School of physics, DAVV, Indore. Abstract One meter long planar undulator i.e. devu20.50p is under fabrication at DAVV, Indore for radiation measurements studies. It will be of PPM type with twenty periods. Each period will be of 50mm. NdFeB magnets will be used with four magnet blocks per period .The size of the NdFeB magnet is 12.5mm x 12.5mm x 50mm. It will be designed with variable gap and tapered gap as well. PPM undulator 4000 a) 3500 3000 2500 Magnetic field (in Gauss) There exist interests in undulators [1] and wigglers for free electron laser. It is proposed to develop a one meter long PPM undulator using NdFeB magnets of 12.5mm × 12.5mm × 50mm at DAVV, Indore. There will be four magnets in each period of length 5cm. There will be twenty periods in the undulator. We will also use half end magnet i.e. 12.5mm×6.25mm×50mm for end field correction. It will be designed with variable uniform gap as well as tapered (Fig 1). 12.5 x 12.5 x 50 mm 1 2 3 4 5 2000 1500 1000 500 0 -500 3000 2500 b) 2000 1500 12.5 x 6.25 x 50 mm 1 2 3 1000 500 0 -500 -0.9 -0.6 -0.3 0.0 0.3 0.6 0.9 Position along the magnet length(in cm) Fig 2 3000 Fig 1 Magnet size 12.5x12.5x50mm 1 2 3 4 5 b) Magnet size 12.5x6.25x50mm 1 2 3 1000 0 Magnetic field (in Gauss) The NdFeB magnets are procured from Shanghai Strong Magnet Industrial & Commercial Co. Ltd, Shanghai, China. The magnet specifications are Grade- N35, Remanence 1.1-1.28T. The measured characterstics of the vertical and horizontal magnets are shown in Fig 2 and Fig 3 respectively. It is proposed to fabricate the lower and upper jaw of the undulaotr. Fig 4a- 4b shows the sample jaw with 5cm long and four magnets are clamped with the tapered clamps. The tapered clamps are preferred in this new design in comparison to old T clamps [2-3]. The clamps for the magnets are tapered at an angle of 15 degree to hold the magnets.The magnet length is 50mm .The jaws are 112 mm in width.The tapered clamps are screwed from the top. Clamp width are 17.7mm each. a) 2000 -1000 -2000 -3000 3000 2000 1000 0 -1000 -2000 -3000 -150 -100 -50 0 50 100 150 Position along the magnet (in mm) Fig 3 --------------------------*The work is supported by DRDO, Delhi, India. Magnet fixure The magnets have to be fixed to the undulator jaws.For this purpose we have developed a special magnet fixture. Fig 5 shows the schematic of magnet fixture. Part (1) is made of brass with two magnetic points. Magnet is attached to part (1) with two magnetic points. On both side of part (1) there are two slots represented by point (2) which can be moved back and forth. These slots are set in front first as shown in the Figure. Now the whole assembly of jaw is placed across the fixer who is designed according to the size of the jaw at point (3). The first magnet is placed manually. By rotating the handle at point (4) the magnet is placed in the jaw, now the slots on either side of the magnet i.e.at point (2) are moved at the back and the magnet is fixed by the clamp on either side of the magnet. Similarly other magnets are placed in the whole assembly. Fig 4a Fig 5 Fig 4b Laser micrometer Conclusion The magnetic field in the undualtor gap is given by π΅(π) = π΅π ππ₯π(βππβππ’ ) (1) Where Br is the remnant field , g is the gap between magnets and ππ’ is one undulator period.Eq (1) tells that the magnetic field inside undulator gap falls exponentially with increased gap. In order to avoid beam wander along the length of the undulator, the gap has to be uniform. It requires perfect size magnets has to be used. We have developed a laser micrometer for non β contact magnet size measurements. In the laser micrometer setup , a laser light from the polygon mirror falls on the magnet. The polygon mirror has eight facets and it can rotate with fixed RPM between 1000-11000. The magnet obstructs some of the light that is collimated at the convex lens. The detector output is connected to a digital storage oscilloscope to read the magnet size. The size of magnets is shown in Fig 6 at a accuracy of 20µm (Fig 6). 12485 Magnet size (inοm) π(ππ) = β50 π΅ ππ ( π π΅π × 10β4 ) (2) B is in Gauss. From Eq. (2), it is predicted that the field variations of 6% corresponds gap variation 1mm. The magnet size are measured by a laser micrometer. Preliminary measurements on some magnets show a size variation of 45µm. We aim to complete the fabrication by this year end. References 12480 12475 a) [1] James A. Clarke, βThe Science and Technology of Undulators and Wigglersβ,Oxford Science Publications. [2] S Tripathi et.al. , Optiocs Communication, 284(2011) 350357. [3] S Tripathi et.al. , Nuclear Instruments and Methods in Physics Research A, 635 (2011)121-126. 12470 12465 12460 12455 12450 RPM 79 = 7978 12445 ο‘ο ο½ο±ο΅ ο° 12440 12435 12430 5 Variation in magnet size (inοm) We have completed the design of the undulator jaws of one meter long undulator. The magnets have been procured. The magnets have been measured by F W Bell 8010Tesla meter. The magnetic measurements are shown in Fig 2. The magnets are chosen randomly. It is observed that the magnets give 3564 Gauss and 3795 Gauss respectively, measured at a distance of 1mm from the magnet surface. This implies a variation of 6%. The end magnets from Fig 2 gives a variation of fields around 2%. The variations in Fig 3 is around 7%. The gap can be calculated from Eq. (1) as for ππ’ = 50ππ , 0 -5 b) -10 -15 -20 -25 RPM 79 = 7978 -30 ο‘ο ο½ο±ο΅ ο° -35 -40 -45 -50 0 2 4 6 8 10 12 14 16 18 Position along the magnet length (in mm) Fig 6 20
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