24 Game - Revision history

en>Mindmatrix: added Category:Year of introduction missing using HotCat

2014-12-15T14:46:13Z

added Category:Year of introduction missing using HotCat

← Older revision		Revision as of 16:46, 15 December 2014
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	~~The writer is recognized by the name of Numbers Lint. My day occupation is a meter reader. Body building is what my family and~~ I ~~enjoy~~. ~~North~~ Dakota is exactly where me and my ~~spouse reside~~.<br><br>~~Take a look at~~ my ~~site :~~: [http://~~rtdcs~~.~~hufs~~.~~ac.kr~~/~~?document_srl=780411~~ home std test]		Nice to meet you, I am Marvella Shryock. South Dakota is exactly where me and my husband live and my family members loves it. Doing ceramics is what adore doing. Managing people has been his day occupation for a whilst.<br><br>Feel free to surf to my website: [http://www.asseryshit.com/groups/valuable-guidance-for-successfully-treating-yeast-infections/ home std test kit]

91.8.131.184: /* Tournament */

2014-02-06T02:32:40Z

Tournament

← Older revision		Revision as of 04:32, 6 February 2014
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	~~'''Spin pumping'''~~ is ~~a method of generating a [[spin current]],~~ the ~~[[spintronics\|spintronic]] analog~~ of ~~a [[battery (electricity)\|battery]] in conventional [[electronics]]~~.		The writer is recognized by the name of Numbers Lint. My day occupation is a meter reader. Body building is what my family and I enjoy. North Dakota is exactly where me and my spouse reside.<br><br>Take a look at my site :: [http://rtdcs.hufs.ac.kr/?document_srl=780411 home std test]

	~~In order to make a spintronic device, the primary requirement~~ is ~~to have~~ a ~~system that can generate a current of spin-polarized [[electrons]], as well as a system that~~ is sensitive to the spin polarization. Most spintronic devices also have a unit in between these two that changes the current of electrons depending on the spin states. Candidates for such devices include injection schemes based on [[magnetic semiconductors]] and ~~[[ferromagnetism\|ferromagnetic]] [[metal]]s, [[ferromagnetic resonance]] devices<ref name=Tserkovnyak>~~
	~~{{Cite journal~~
	~~\| title = Enhanced Gilbert Damping in Thin Ferromagnetic Films~~
	~~\| year = 2002~~
	~~\| volume = 88 \| issue = 11~~
	~~\| author = Y Tserkovnyak et al~~
	~~\| journal = Physical Review Letters~~
	~~\| doi = 10~~.~~1103/PhysRevLett.88.117601~~
	~~\| bibcode=2002PhRvL..88k7601T~~
	~~\|arxiv = cond-mat/0110247 }}</ref>~~
	, and ~~a variety of [[spin-dependent pump]]s~~. ~~Optical, microwave and electrical methods are also being explored~~<~~ref~~>
	~~{{Cite journal~~
	~~\| title = Spin Pumping by Parametrically Excited Exchange Magnons~~
	~~\| year = 2011~~
	~~\| volume = 106 \| page = 216601~~
	~~\| author = C Sandweg et al~~
	~~\| journal = Physical Review Letters~~
	~~\| doi = 10.1103/PhysRevLett.106.216601~~
	~~\| bibcode=2011PhRvL.106u6601S~~
	~~\|arxiv = 1103.2229 }}~~<~~/ref~~>
	~~.These devices could be used for low-power data transmission in~~ [~~[spintronic]] devices<ref>~~
	~~{{Cite journal~~
	~~\| title = Spin-magnon transmutation~~
	~~\| year = 2011~~
	~~\| volume = 4 \| page = 40~~
	~~\| author = G E Bauer and Y Tserkovnyak~~
	~~\| journal = Physics~~
	~~\| doi = 10.1103~~/~~Physics.4.40~~
	~~\|bibcode = 2011PhyOJ...4...40B }}<~~/~~ref>~~
	~~or to transmit electrical signals through insulators~~.~~<ref>~~
	~~{{Cite journal~~
	~~\| title = Transmission of electrical signals by spin-wave interconversion in a magnetic insulator~~
	~~\| year = 2010~~
	~~\| volume = 464~~
	~~\| author = Y Kajiwara~~
	~~\| journal = Nature~~
	~~\| doi = 10~~.~~1038/nature08876~~
	~~\| issue=7286~~
	~~\|bibcode = 2010Natur~~.~~464..262K }}</ref>~~

	~~The spin pumped into an adjacent layer by a precessing magnetic moment is given by<ref name=Tserkovnyak/>~~
	~~:<math>\vec j_s = {\hbar \over {4 \pi}} g^{\uparrow \downarrow} {1 \over M_S^2} \langle \vec M(t) \times {{d \vec M(t))} \over {dt}} \rangle </math>~~
	where <math>\vec j_s</math> is the spin current (the vector indicates the orientation of the spin, ''not'' the direction of the current), <math>g^{\uparrow \downarrow}</math> is the spin-mixing conductance, <math> M_S^2</~~math> is the saturation magnetization, and <math>\vec M(t)</math> is the time-dependent orientation of the moment.~~

	~~==References==~~
	~~{{Reflist}}~~

	~~==See also~~==
	*[[Spintronic]]
	*[[Spin wave]]
	*[[Spin Engineering]]
	*[[Spin Hall effect]]

	~~{{DEFAULTSORT:Spin Pumping}}~~
	~~[[Category:Spintronics]~~]


	~~{{Physics-stub}}~~

en>Mindmatrix: add Category:Card games introduced in the 1960s; formatting: 3x heading-style, 2x whitespace (using Advisor.js)

2014-01-22T02:21:47Z

add Category:Card games introduced in the 1960s; formatting: 3x heading-style, 2x whitespace (using Advisor.js)

← Older revision		Revision as of 04:21, 22 January 2014
Line 1:		Line 1:
	~~Hello and welcome~~. ~~My title~~ is ~~Irwin~~ and ~~I totally dig that~~ name. ~~To gather cash is what his family~~ and ~~him appreciate~~. ~~Bookkeeping is my profession~~. ~~Puerto Rico is exactly where he~~ and ~~his spouse live~~.<br><br>~~Look into my blog post~~ ... ~~[http~~://~~www.reachoutsociety.info~~/~~blog~~/~~435 home std test~~]		'''Spin pumping''' is a method of generating a [[spin current]], the [[spintronics\|spintronic]] analog of a [[battery (electricity)\|battery]] in conventional [[electronics]].

			In order to make a spintronic device, the primary requirement is to have a system that can generate a current of spin-polarized [[electrons]], as well as a system that is sensitive to the spin polarization. Most spintronic devices also have a unit in between these two that changes the current of electrons depending on the spin states. Candidates for such devices include injection schemes based on [[magnetic semiconductors]] and [[ferromagnetism\|ferromagnetic]] [[metal]]s, [[ferromagnetic resonance]] devices<ref name=Tserkovnyak>
			{{Cite journal
			\| title = Enhanced Gilbert Damping in Thin Ferromagnetic Films
			\| year = 2002
			\| volume = 88 \| issue = 11
			\| author = Y Tserkovnyak et al
			\| journal = Physical Review Letters
			\| doi = 10.1103/PhysRevLett.88.117601
			\| bibcode=2002PhRvL..88k7601T
			\|arxiv = cond-mat/0110247 }}</ref>
			, and a variety of [[spin-dependent pump]]s. Optical, microwave and electrical methods are also being explored<ref>
			{{Cite journal
			\| title = Spin Pumping by Parametrically Excited Exchange Magnons
			\| year = 2011
			\| volume = 106 \| page = 216601
			\| author = C Sandweg et al
			\| journal = Physical Review Letters
			\| doi = 10.1103/PhysRevLett.106.216601
			\| bibcode=2011PhRvL.106u6601S
			\|arxiv = 1103.2229 }}</ref>
			.These devices could be used for low-power data transmission in [[spintronic]] devices<ref>
			{{Cite journal
			\| title = Spin-magnon transmutation
			\| year = 2011
			\| volume = 4 \| page = 40
			\| author = G E Bauer and Y Tserkovnyak
			\| journal = Physics
			\| doi = 10.1103/Physics.4.40
			\|bibcode = 2011PhyOJ...4...40B }}</ref>
			or to transmit electrical signals through insulators.<ref>
			{{Cite journal
			\| title = Transmission of electrical signals by spin-wave interconversion in a magnetic insulator
			\| year = 2010
			\| volume = 464
			\| author = Y Kajiwara
			\| journal = Nature
			\| doi = 10.1038/nature08876
			\| issue=7286
			\|bibcode = 2010Natur.464..262K }}</ref>

			The spin pumped into an adjacent layer by a precessing magnetic moment is given by<ref name=Tserkovnyak/>
			:<math>\vec j_s = {\hbar \over {4 \pi}} g^{\uparrow \downarrow} {1 \over M_S^2} \langle \vec M(t) \times {{d \vec M(t))} \over {dt}} \rangle </math>
			where <math>\vec j_s</math> is the spin current (the vector indicates the orientation of the spin, ''not'' the direction of the current), <math>g^{\uparrow \downarrow}</math> is the spin-mixing conductance, <math> M_S^2</math> is the saturation magnetization, and <math>\vec M(t)</math> is the time-dependent orientation of the moment.

			==References==
			{{Reflist}}

			==See also==
			*[[Spintronic]]
			*[[Spin wave]]
			*[[Spin Engineering]]
			*[[Spin Hall effect]]

			{{DEFAULTSORT:Spin Pumping}}
			[[Category:Spintronics]]


			{{Physics-stub}}

108.6.2.138 at 15:09, 28 August 2012

2012-08-28T15:09:58Z

New page

Hello and welcome. My title is Irwin and I totally dig that name. To gather cash is what his family and him appreciate. Bookkeeping is my profession. Puerto Rico is exactly where he and his spouse live.<br><br>Look into my blog post ... [http://www.reachoutsociety.info/blog/435 home std test]

← Older revision		Revision as of 04:32, 6 February 2014
Line 1:		Line 1:
	~~'''Spin pumping'''~~ is ~~a method of generating a [[spin current]],~~ the ~~[[spintronics\|spintronic]] analog~~ of ~~a [[battery (electricity)\|battery]] in conventional [[electronics]]~~.		The writer is recognized by the name of Numbers Lint. My day occupation is a meter reader. Body building is what my family and I enjoy. North Dakota is exactly where me and my spouse reside.<br><br>Take a look at my site :: [http://rtdcs.hufs.ac.kr/?document_srl=780411 home std test]

	~~In order to make a spintronic device, the primary requirement~~ is ~~to have~~ a ~~system that can generate a current of spin-polarized [[electrons]], as well as a system that~~ is sensitive to the spin polarization. Most spintronic devices also have a unit in between these two that changes the current of electrons depending on the spin states. Candidates for such devices include injection schemes based on [[magnetic semiconductors]] and ~~[[ferromagnetism\|ferromagnetic]] [[metal]]s, [[ferromagnetic resonance]] devices<ref name=Tserkovnyak>~~
	~~{{Cite journal~~
	~~\| title = Enhanced Gilbert Damping in Thin Ferromagnetic Films~~
	~~\| year = 2002~~
	~~\| volume = 88 \| issue = 11~~
	~~\| author = Y Tserkovnyak et al~~
	~~\| journal = Physical Review Letters~~
	~~\| doi = 10~~.~~1103/PhysRevLett.88.117601~~
	~~\| bibcode=2002PhRvL..88k7601T~~
	~~\|arxiv = cond-mat/0110247 }}</ref>~~
	, and ~~a variety of [[spin-dependent pump]]s~~. ~~Optical, microwave and electrical methods are also being explored~~<~~ref~~>
	~~{{Cite journal~~
	~~\| title = Spin Pumping by Parametrically Excited Exchange Magnons~~
	~~\| year = 2011~~
	~~\| volume = 106 \| page = 216601~~
	~~\| author = C Sandweg et al~~
	~~\| journal = Physical Review Letters~~
	~~\| doi = 10.1103/PhysRevLett.106.216601~~
	~~\| bibcode=2011PhRvL.106u6601S~~
	~~\|arxiv = 1103.2229 }}~~<~~/ref~~>
	~~.These devices could be used for low-power data transmission in~~ [~~[spintronic]] devices<ref>~~
	~~{{Cite journal~~
	~~\| title = Spin-magnon transmutation~~
	~~\| year = 2011~~
	~~\| volume = 4 \| page = 40~~
	~~\| author = G E Bauer and Y Tserkovnyak~~
	~~\| journal = Physics~~
	~~\| doi = 10.1103~~/~~Physics.4.40~~
	~~\|bibcode = 2011PhyOJ...4...40B }}<~~/~~ref>~~
	~~or to transmit electrical signals through insulators~~.~~<ref>~~
	~~{{Cite journal~~
	~~\| title = Transmission of electrical signals by spin-wave interconversion in a magnetic insulator~~
	~~\| year = 2010~~
	~~\| volume = 464~~
	~~\| author = Y Kajiwara~~
	~~\| journal = Nature~~
	~~\| doi = 10~~.~~1038/nature08876~~
	~~\| issue=7286~~
	~~\|bibcode = 2010Natur~~.~~464..262K }}</ref>~~

	~~The spin pumped into an adjacent layer by a precessing magnetic moment is given by<ref name=Tserkovnyak/>~~
	~~:<math>\vec j_s = {\hbar \over {4 \pi}} g^{\uparrow \downarrow} {1 \over M_S^2} \langle \vec M(t) \times {{d \vec M(t))} \over {dt}} \rangle </math>~~
	where <math>\vec j_s</math> is the spin current (the vector indicates the orientation of the spin, ''not'' the direction of the current), <math>g^{\uparrow \downarrow}</math> is the spin-mixing conductance, <math> M_S^2</~~math> is the saturation magnetization, and <math>\vec M(t)</math> is the time-dependent orientation of the moment.~~

	~~==References==~~
	~~{{Reflist}}~~

	~~==See also~~==
	*[[Spintronic]]
	*[[Spin wave]]
	*[[Spin Engineering]]
	*[[Spin Hall effect]]

	~~{{DEFAULTSORT:Spin Pumping}}~~
	~~[[Category:Spintronics]~~]


	~~{{Physics-stub}}~~