Fixing of photorefractive gratings in KLTN by a 4 K cooldown to the phase transition

Summary form only given. In crystals of potassium lithium tantalate niobate (KLTN), we observed that as the crystals are cooled to the phase transition there is an increase in the conductivity, which disappears immediately below the transition. This fact was the basis to the following holographic fi...

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Hauptverfasser: Razvag, M., Balberg, M., Agranat, A.J.
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description Summary form only given. In crystals of potassium lithium tantalate niobate (KLTN), we observed that as the crystals are cooled to the phase transition there is an increase in the conductivity, which disappears immediately below the transition. This fact was the basis to the following holographic fixing process: First, a photorefractive (PR) space charge hologram is written in the crystal in the region where the conductivity is low, at 4 K above T/sub c/. The crystal is then cooled to the phase transition and then warmed up to its initial temperature. Finally an erasing beam is incident on the crystal until the space charge grating is erased. It was predicted that because the ionic species become mobile at the phase transition, a compensation of the PR space charge will occur. The ions will be frozen when the crystal is heated to its original temperature. Thus, after the PR space charge is erased, the frozen space charge will be exposed and the hologram it represents will remain fixed. This process was tested in a KLTN crystal with T/sub c/=170 K, doped with copper and vanadium.
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In crystals of potassium lithium tantalate niobate (KLTN), we observed that as the crystals are cooled to the phase transition there is an increase in the conductivity, which disappears immediately below the transition. This fact was the basis to the following holographic fixing process: First, a photorefractive (PR) space charge hologram is written in the crystal in the region where the conductivity is low, at 4 K above T/sub c/. The crystal is then cooled to the phase transition and then warmed up to its initial temperature. Finally an erasing beam is incident on the crystal until the space charge grating is erased. It was predicted that because the ionic species become mobile at the phase transition, a compensation of the PR space charge will occur. The ions will be frozen when the crystal is heated to its original temperature. Thus, after the PR space charge is erased, the frozen space charge will be exposed and the hologram it represents will remain fixed. This process was tested in a KLTN crystal with T/sub c/=170 K, doped with copper and vanadium.</description><identifier>ISBN: 1557524432</identifier><identifier>ISBN: 9781557524430</identifier><language>eng</language><publisher>IEEE</publisher><subject>Conductivity ; Crystals ; Gratings ; Holography ; Lithium compounds ; Niobium compounds ; Photorefractive effect ; Photorefractive materials ; Space charge ; Temperature</subject><ispartof>Summaries of papers presented at the Conference on Lasers and Electro-Optics, 1996, p.71</ispartof><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/864371$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>310,311,782,786,791,792,2060,4052,4053,54927</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/864371$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Razvag, M.</creatorcontrib><creatorcontrib>Balberg, M.</creatorcontrib><creatorcontrib>Agranat, A.J.</creatorcontrib><title>Fixing of photorefractive gratings in KLTN by a 4 K cooldown to the phase transition</title><title>Summaries of papers presented at the Conference on Lasers and Electro-Optics</title><addtitle>CLEO</addtitle><description>Summary form only given. In crystals of potassium lithium tantalate niobate (KLTN), we observed that as the crystals are cooled to the phase transition there is an increase in the conductivity, which disappears immediately below the transition. This fact was the basis to the following holographic fixing process: First, a photorefractive (PR) space charge hologram is written in the crystal in the region where the conductivity is low, at 4 K above T/sub c/. The crystal is then cooled to the phase transition and then warmed up to its initial temperature. Finally an erasing beam is incident on the crystal until the space charge grating is erased. It was predicted that because the ionic species become mobile at the phase transition, a compensation of the PR space charge will occur. The ions will be frozen when the crystal is heated to its original temperature. Thus, after the PR space charge is erased, the frozen space charge will be exposed and the hologram it represents will remain fixed. This process was tested in a KLTN crystal with T/sub c/=170 K, doped with copper and vanadium.</description><subject>Conductivity</subject><subject>Crystals</subject><subject>Gratings</subject><subject>Holography</subject><subject>Lithium compounds</subject><subject>Niobium compounds</subject><subject>Photorefractive effect</subject><subject>Photorefractive materials</subject><subject>Space charge</subject><subject>Temperature</subject><isbn>1557524432</isbn><isbn>9781557524430</isbn><fulltext>true</fulltext><rsrctype>conference_proceeding</rsrctype><creationdate>1996</creationdate><recordtype>conference_proceeding</recordtype><sourceid>6IE</sourceid><sourceid>RIE</sourceid><recordid>eNp9i8sKwjAQAAMi-OoPeNofEGybtN7FIlQ89V5i3bYrNVuSoPbvzcGzc5nDMDOxipXKVSJlmixE5NxjH5AqlplaiqqgD5kOuIWxZ88WW6sbTy-EzmofkgMyUF6qK9wm0CChhIZ5uPPbgGfwPYZTOwRvtXHkic1GzFs9OIx-XottcaqO5x0hYj1aemo71YdMpnmc_o1fwaw5cg</recordid><startdate>1996</startdate><enddate>1996</enddate><creator>Razvag, M.</creator><creator>Balberg, M.</creator><creator>Agranat, A.J.</creator><general>IEEE</general><scope>6IE</scope><scope>6IL</scope><scope>CBEJK</scope><scope>RIE</scope><scope>RIL</scope></search><sort><creationdate>1996</creationdate><title>Fixing of photorefractive gratings in KLTN by a 4 K cooldown to the phase transition</title><author>Razvag, M. ; Balberg, M. ; Agranat, A.J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-ieee_primary_8643713</frbrgroupid><rsrctype>conference_proceedings</rsrctype><prefilter>conference_proceedings</prefilter><language>eng</language><creationdate>1996</creationdate><topic>Conductivity</topic><topic>Crystals</topic><topic>Gratings</topic><topic>Holography</topic><topic>Lithium compounds</topic><topic>Niobium compounds</topic><topic>Photorefractive effect</topic><topic>Photorefractive materials</topic><topic>Space charge</topic><topic>Temperature</topic><toplevel>online_resources</toplevel><creatorcontrib>Razvag, M.</creatorcontrib><creatorcontrib>Balberg, M.</creatorcontrib><creatorcontrib>Agranat, A.J.</creatorcontrib><collection>IEEE Electronic Library (IEL) Conference Proceedings</collection><collection>IEEE Proceedings Order Plan All Online (POP All Online) 1998-present by volume</collection><collection>IEEE Xplore All Conference Proceedings</collection><collection>IEEE Electronic Library (IEL)</collection><collection>IEEE Proceedings Order Plans (POP All) 1998-Present</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Razvag, M.</au><au>Balberg, M.</au><au>Agranat, A.J.</au><format>book</format><genre>proceeding</genre><ristype>CONF</ristype><atitle>Fixing of photorefractive gratings in KLTN by a 4 K cooldown to the phase transition</atitle><btitle>Summaries of papers presented at the Conference on Lasers and Electro-Optics</btitle><stitle>CLEO</stitle><date>1996</date><risdate>1996</risdate><spage>71</spage><pages>71-</pages><isbn>1557524432</isbn><isbn>9781557524430</isbn><abstract>Summary form only given. In crystals of potassium lithium tantalate niobate (KLTN), we observed that as the crystals are cooled to the phase transition there is an increase in the conductivity, which disappears immediately below the transition. This fact was the basis to the following holographic fixing process: First, a photorefractive (PR) space charge hologram is written in the crystal in the region where the conductivity is low, at 4 K above T/sub c/. The crystal is then cooled to the phase transition and then warmed up to its initial temperature. Finally an erasing beam is incident on the crystal until the space charge grating is erased. It was predicted that because the ionic species become mobile at the phase transition, a compensation of the PR space charge will occur. The ions will be frozen when the crystal is heated to its original temperature. Thus, after the PR space charge is erased, the frozen space charge will be exposed and the hologram it represents will remain fixed. This process was tested in a KLTN crystal with T/sub c/=170 K, doped with copper and vanadium.</abstract><pub>IEEE</pub></addata></record>
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identifier ISBN: 1557524432
ispartof Summaries of papers presented at the Conference on Lasers and Electro-Optics, 1996, p.71
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source IEEE Electronic Library (IEL) Conference Proceedings
subjects Conductivity
Crystals
Gratings
Holography
Lithium compounds
Niobium compounds
Photorefractive effect
Photorefractive materials
Space charge
Temperature
title Fixing of photorefractive gratings in KLTN by a 4 K cooldown to the phase transition
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