Geometric design of roads - Revision history

en>IceKarma: Reverted edits by 66.56.191.72 (talk) to last version by Timpo

2014-10-29T14:57:36Z

Reverted edits by 66.56.191.72 (talk) to last version by Timpo

← Older revision		Revision as of 16:57, 29 October 2014
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	~~I’m Aurelio~~ from ~~Gouda studying Integrated International Studies~~. ~~I did my schooling~~, ~~secured 91%~~ and ~~hope~~ to ~~find someone with same interests~~ in ~~Stamp collecting~~.<br><br>~~Take~~ a ~~look~~ at ~~my blog post~~ - [http://~~www~~.~~slideshare~~.~~net~~/~~davnec samsung galaxy note~~ 4 ~~manual t~~-~~mobile]~~		Captain America, Spideг-Man, the X-Men and Transformers are ѕtorming back into movie theateгs, retսrning in [http://search.Usa.gov/search?query=sequels sequels] to save the world from mass destruction, while at the same time chսrning out profits for movie studios.<br><br>Hollyաood will pack 13 ѕequels into theaters over the next 20 weeks. Tɦe parade begins on Friday, when Сaptain America dons his red-whitе-and-blue superhero suit foг the U.S. debսt of Marvel'ѕ "Captain America: The Winter Soldier," and continueѕ thrߋugɦ summer, Hollywߋod's mօst lucrative sеason.<br><br>Stuԁios generally don't have to sрend as muϲh to raise awaгeness of sequels months in adѵance, as they do ѡith other big-budget films, executives say. And աhen [http://Photobucket.com/images/sequels+reach sequels reach] tɦe Ƅig screen, ticket sales in foreign mаrkets, which can account for up to 80 percent of a film's box office, often exceed their predecessors.<br><br>"When you can say, here's 'Avatar 2,' and you've got six billion people ready to see it, it doesn't take a lot of marketing to get them into the theater," said Jim Gianopulos, chairmаn and chief еxecutive of Fߋx Filmed Entertainment. "It's a self-propelling marketing message in a very big world."<br><br>The first installment of 20th Century Fox's animated "Ice Age" series took in $207 milliοn overseas in 2002. The fourth "Ice Age" from the stuɗio owned bʏ Ƭwenty-First Century Fox earned $716 million at international box officeѕ in 2012.<br>Sequels are hardly a new Hollywood phenomenon. But in recent years, as DVD sales сrumbled, movie studioѕ began to cut back on the numbers of films tɦey produced to trim the risҟs.<br>Stɑrting in 2008, they began to chuгn out more sequels and big-budget event films, turning away from riskier origіnal films like independent dramаs and romantic comedies.<br><br>This year's sequels include superhero films "The Amazing Spider-Man 2" from Sony Corp, Fox's "X-Men: Days of Future Past," аnd "Transformers: Age of Extinction" from Viacom Inc'ѕ Paramount; animated movies "Rio 2" from Fox and Ɗreamworks Αnimation's "How to Train Your Dragon 2;" and Sony comedieѕ "22 Jump Street" and "Think Like a Man Too."<br>What mostly drives the studio top brass is that audiences keep buying ticкets for sequels. In 2013, nine of [http://theamazingspider-Man2Movie.blogspot.com/ watch the Amazing spider-man 2 full movie] top 12 films іn the U.S. and Canada were sequels or pгequels, including Marvel's "Iron Man 3" and Lions Gatе's "The Hunger Games: Catching Fire." Those films geneгated $2.6 billion in domestic ticket sales, nearly one-quarter of the year's $10.9 billion total, and another $4.5 billion ԝorldwide.<br><br>That shift away from riskier films has helpеd studios increase or stabilize their profits, said Jannеy Montgomery Scott analyst Tony Wible.<br>Оperating margins at Time Warneг Inc's Warner Bros., tҺe studio behind the "Harry Potter" franchise and "The Dark Knight" Batman series, hovered around 7 percent in 2007 and 2008, Ԝible sаid, beforе rising to about 10 peгcent for eɑch of the next five years.<br><br>At Walt Ɗisneу Co, the focus is on a smaller number of films with the pօtential to proɗucе sequels, drive toy ѕɑles and inspire theme-park rides.<br><br>In a typical year, Ɗisney is aiming to release one film each from Pixar, Disney Animɑtion, and "Star Wars" producer Lucasfilm; twο from Marѵel, and four to six from its Disney live action division, said Alan Horn, chairman of The Walt Ɗisney Stuɗios. "We choose our sequels carefully," Horn said.<br>"If we have a picture that has earned a right to have a sequel, it's because the audiences loved it."<br>Next year's crop of sequels may set even bigger recoгds. Studіos are already ƿlanning to release new іnstallments of some of the biggest films of ɑll time, including "Star Wars," "Jurassic Park" and "Marvel's The Avengers."<br><br>The rash of sequels has prompted even filmmakers to make fun of theіr world. In the opening number for "Muppets Most Wanted," Disney's ѕequel to itѕ 2011 "The Muppets" movie, the furry puppеts break into a song cɑlled "We're Doing a Sequel."<br>"That's what we do in Hollywood," the puƿpets sing, "and everybody knows that the sequel's never quite as good."<br>(Reporting by Lisa Richwine; Editіng by Ronald Grover and Kenneth Maxwell)

en>BG19bot: /* Cross slope */WP:CHECKWIKI error fix for #61. Punctuation goes before References. Do general fixes if a problem exists. - using AWB (9916)

2014-02-07T05:51:06Z

Cross slope: WP:CHECKWIKI error fix for #61. Punctuation goes before References. Do general fixes if a problem exists. - using AWB (9916)

← Older revision		Revision as of 07:51, 7 February 2014
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	'''Free carrier absorption''' occurs when a material absorbs a photon and a carrier is excited from a filled state to an unoccupied state (in the same band). This is different from interband absorption in semiconductors because the excited electron is a conduction electron (i.e. it can move freely). In interband absorption the electron in question would be raised from ~~a valence (nonconducting) band to a conducting one~~.		I’m Aurelio from Gouda studying Integrated International Studies. I did my schooling, secured 91% and hope to find someone with same interests in Stamp collecting.<br><br>Take a look at my blog post - [http://www.slideshare.net/davnec samsung galaxy note 4 manual t-mobile]

	It is well known that the optical transition of electrons and [[Electron hole\|hole]]s in the solid state is a useful clue to understand the physical properties of the material. However, the dynamics of the [[Charge carrier\|carrier]] is affected by other carriers, not only by the periodic lattice potential. Moreover, the thermal fluctuation of each electron should be taken into account. Therefore a statistical approach is needed. To predict the optical transition in an appropriate precession, one should choose an approximation, called assumption of quasi-thermal distributions, of the electrons in the conduction band and ~~of the holes in the valence band. In this case, the diagonal components of the [[density matrix]] become negligible after introducing thermal distribution function,~~

	~~<math>\rho _{\lambda \lambda }^0 = \frac{1}{{e^{(\varepsilon _{\lambda ,k} - \mu )\beta } + 1}} = f_{\lambda ,k}</math>~~

	~~This is the famous [[Fermi dirac statistics\|Fermi-Dirac distribution]] for the distribution of electron energies. Thus, summing over possible l and k yields the total number of carriers N.~~

	~~<math>N_\lambda = \sum\limits_\lambda {f_{\lambda ,k}}</math>~~

	~~==The optical susceptibility==~~

	~~Using the above distribution function, the time evolution of density matrix does not have~~ to ~~be solved and the complexity is simplified.~~

	<math> \rho _{cv}^{{\mathop{\rm int}} } (k,t) = \int {\frac{{d\omega }}{{2\pi }}\frac{{d_{cv} \varepsilon (\omega )e^{i(\varepsilon _{c,k} - \varepsilon _{v,k} - \omega )t} }}{{\hbar (\varepsilon _{c,k} - \varepsilon _{v,k} - \omega - i\gamma )}}(f_{v,k} - f_{c,k} )}</math>

	~~The optical polarization is,~~

	~~<math>\displaystyle P(t) = tr[\rho (t)d]</math>~~

	~~With this relation and after adjusting the Fourier transformation, the optical susceptibility is~~
	<math>\chi (\omega ) = - \sum\limits_k {\frac{{\left\| {d_{cv} } \right\|^{_2 } }}{{L^3 }}} (f_{v,k} - f_{c,k})\left( {\frac{1}{{\hbar (\varepsilon _{v,k} - \varepsilon _{c,k}+ \omega + i\gamma )}} - \frac{1}{{\hbar (\varepsilon _{c,k} - \varepsilon _{v,k} + \omega + i\gamma )}}} \right)</math>

	~~==Absorption coefficient==~~

	The transition amplitude corresponds to the absorption of energy and the absorbed energy is proportional to the optical conductivity which is the imaginary part of the optical susceptibility after frequency is multiplied. Therefore, in ~~order to obtain the absorption coefficient that is crucial quantity for investigation of electronic structure, we can use the optical susceptibility~~.

	<~~math~~> ~~\alpha (\omega ) = \frac{{4\pi \omega }}{{n_b c}}\chi ''(\omega )~~<~~/math~~>

	~~<math>{\rm{ }} = \frac{{4\pi \omega }}{{n_b c}}\sum\limits_k {\left\| {d_{cv} } \right\|^2 (f_{v,k}~~ - ~~f_{c,k} )\delta (\hbar (\varepsilon _{v,k} - \varepsilon _{c,k} + \omega ))}</math>~~

	Considering the gap energy Eg, energy dispersion relation of free carrier proportional to the square of momentum and the relation of electron-hole distribution function, we can obtain the absorption coefficient with some kind of mathematical calculation. The final result is
	<math>\alpha (\omega ) = \alpha _0^d \frac{{\hbar \omega }}{{E_0 }}\left( {\frac{{\hbar \omega - E_g - E_0^{(d)} }}{{E_0 }}} \right)^{(d - 2)/2} \sum\limits_k {\Theta (\hbar \omega - E_g - E_0^{(d)} )A(\omega )} </math>

	The application of this result to semiconductor is important to understand the optical measurement data and the electronic properties. Some example shows the negative absorption coefficient that is fundamental presentation of [[Laser diode\|semiconductor laser]].

	~~==References==~~
	~~1. H. Haug and S. W. Koch, "~~[http://~~books.google~~.co.kr/~~books?id=~~-UoG0Hx0w04C&dq=Quantum+Theory+of+the+Optical+and+Electronic+Properties+of+Semiconductors&printsec=frontcover&source=bn&hl=ko&ei=DoneSeT7Ipne7APqv6AJ&sa=X&oi=book_result&ct=result&resnum=5 Quantum Theory of the Optical and Electronic Properties of Semiconductors]
	~~", World Scientific (1994). sec.5.4 a~~

	~~[[Category:Quantum mechanics]~~]

en>Triskele Jim: Undid revision 593259833 by 59.97.26.183 (talk) rmcommercial link

2014-01-31T17:45:17Z

Undid revision 593259833 by 59.97.26.183 (talk) rmcommercial link

← Older revision		Revision as of 19:45, 31 January 2014
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	~~Hi there! :~~) [~~http://www~~.~~metasilicatos~~.~~net~~/~~%E6%B4%92%E8%90%BD%E3%81%AA~~-~~%E6%B0%B4%E6%B3%B3-%E3%82%AA%E3%83%B3%E3%83%A9%E3%82%A4%E3%83%B3%E3%82%B7%E3%83%A7%E3%83%83%E3%83%97~~/~~%E5%A4%A7%E5%A5%BD%E8%A9%95~~-~~%E3%82%B9%E3%82%A4%E3%83%A0%E3%82%A6%E3%82%A7%E3%82%A2~~-~~%E3%83%A1%E3%83%B3%E3%82%BA~~-~~%E6%B0%97%E8%B3%AA%E3%82%A2%E3%83%83%E3%83%97/%E6%B4%97%E7%B7%B4%E3%81%95%E3%82%8C%E3%81%9F~~-~~%E3%82%B9%E3%82%A4%E3%83%A0%E3%82%A4%E3%83%B3%E3%83%8A%E3%83%BC~~-~~%E3%82%AA%E3%83%B3%E3%83%A9%E3%82%A4%E3%83%B3%E5%BA%97 水泳スイムインナー]~~ [~~http:~~/~~/www.metasilicatos.net/%E5%90%84%E5%BF%85%E8%A6%81%E3%82%92%E6%BA%80%E8%B6%B3%E3%81%99%E3%82%8B~~-~~%E3%82%A2%E3%82%A6%E3%83%88%E3%83%89%E3%82%A2~~-~~%E9%80%9A%E8%B2%A9/%E7%BE%8E%E3%81%97%E3%81%84~~-~~%E6%B0%B4%E3%82%BF%E3%83%B3%E3%82%AF%E3%83%BB%E3%83%9D%E3%83%AA%E3%82%BF%E3%83%B3%E3%82%AF~~-~~%E6%B3%A8%E6%96%87%E5%89%B2%E5%BC%95%E9%96%8B%E5%82%AC%E4%B8%AD アウトドア水タンクポリタンク] My name is Claudette~~, ~~I'm a student studying Agriculture~~ ~~[http:~~/~~/www~~.~~metasilicatos~~.~~net~~/~~%E6%B4%92%E8%90%BD%E3%81%AA~~-~~%E6%B0%B4%E6%B3%B3~~-~~%E3%82%AA%E3%83%B3%E3%83%A9%E3%82%A4%E3%83%B3%E3%82%B7%E3%83%A7%E3%83%83%E3%83%97~~/~~%E4%B8%8A%E5%93%81-%E3%82%A2%E3%82%AF%E3%82%A2%E3%83%95%E3%82%A9%E3%83%BC%E3%82%B9%E3%83%BB%E3%83%95%E3%83%A5%E3%83%BC%E3%82%B8%E3%83%A7%E3%83%B3~~-~~%E8%B4%88%E5%91%88 水泳アクアフォースフュージョン] and Life Sciences from Vordingborg~~, ~~Denmark~~.<br><br>~~Review my web-site -~~ [http://~~www~~.~~metasilicatos~~.~~net~~/~~%E3%82%AA%E3%83%B3%E3%83%A9%E3%82%A4%E3%83%B3%E3%82%B7%E3%83%A7%E3%83%83%E3%83%97~~-%E3%83%95%E3%82%A3%E3%83%83%E3%82%B7%E3%83%B3%E3%82%B0-%E9%80%9A%E8%B2%A9/%E6%B4%92%E8%90%BD%E3%81%AA-%E6%8A%95%E7%AB%BF-%E5%AE%9A%E7%95%AA/%E5%A4%A7%E4%BA%BA%E6%B0%97-%E3%82%B7%E3%83%9E%E3%83%8E-%E5%AE%9A%E7%95%AA フィッシングシマノ]		'''Free carrier absorption''' occurs when a material absorbs a photon and a carrier is excited from a filled state to an unoccupied state (in the same band). This is different from interband absorption in semiconductors because the excited electron is a conduction electron (i.e. it can move freely). In interband absorption the electron in question would be raised from a valence (nonconducting) band to a conducting one.

			It is well known that the optical transition of electrons and [[Electron hole\|hole]]s in the solid state is a useful clue to understand the physical properties of the material. However, the dynamics of the [[Charge carrier\|carrier]] is affected by other carriers, not only by the periodic lattice potential. Moreover, the thermal fluctuation of each electron should be taken into account. Therefore a statistical approach is needed. To predict the optical transition in an appropriate precession, one should choose an approximation, called assumption of quasi-thermal distributions, of the electrons in the conduction band and of the holes in the valence band. In this case, the diagonal components of the [[density matrix]] become negligible after introducing thermal distribution function,

			<math>\rho _{\lambda \lambda }^0 = \frac{1}{{e^{(\varepsilon _{\lambda ,k} - \mu )\beta } + 1}} = f_{\lambda ,k}</math>

			This is the famous [[Fermi dirac statistics\|Fermi-Dirac distribution]] for the distribution of electron energies. Thus, summing over possible l and k yields the total number of carriers N.

			<math>N_\lambda = \sum\limits_\lambda {f_{\lambda ,k}}</math>

			==The optical susceptibility==

			Using the above distribution function, the time evolution of density matrix does not have to be solved and the complexity is simplified.

			<math> \rho _{cv}^{{\mathop{\rm int}} } (k,t) = \int {\frac{{d\omega }}{{2\pi }}\frac{{d_{cv} \varepsilon (\omega )e^{i(\varepsilon _{c,k} - \varepsilon _{v,k} - \omega )t} }}{{\hbar (\varepsilon _{c,k} - \varepsilon _{v,k} - \omega - i\gamma )}}(f_{v,k} - f_{c,k} )}</math>

			The optical polarization is,

			<math>\displaystyle P(t) = tr[\rho (t)d]</math>

			With this relation and after adjusting the Fourier transformation, the optical susceptibility is
			<math>\chi (\omega ) = - \sum\limits_k {\frac{{\left\| {d_{cv} } \right\|^{_2 } }}{{L^3 }}} (f_{v,k} - f_{c,k})\left( {\frac{1}{{\hbar (\varepsilon _{v,k} - \varepsilon _{c,k}+ \omega + i\gamma )}} - \frac{1}{{\hbar (\varepsilon _{c,k} - \varepsilon _{v,k} + \omega + i\gamma )}}} \right)</math>

			==Absorption coefficient==

			The transition amplitude corresponds to the absorption of energy and the absorbed energy is proportional to the optical conductivity which is the imaginary part of the optical susceptibility after frequency is multiplied. Therefore, in order to obtain the absorption coefficient that is crucial quantity for investigation of electronic structure, we can use the optical susceptibility.

			<math> \alpha (\omega ) = \frac{{4\pi \omega }}{{n_b c}}\chi ''(\omega )</math>

			<math>{\rm{ }} = \frac{{4\pi \omega }}{{n_b c}}\sum\limits_k {\left\| {d_{cv} } \right\|^2 (f_{v,k} - f_{c,k} )\delta (\hbar (\varepsilon _{v,k} - \varepsilon _{c,k} + \omega ))}</math>

			Considering the gap energy Eg, energy dispersion relation of free carrier proportional to the square of momentum and the relation of electron-hole distribution function, we can obtain the absorption coefficient with some kind of mathematical calculation. The final result is
			<math>\alpha (\omega ) = \alpha _0^d \frac{{\hbar \omega }}{{E_0 }}\left( {\frac{{\hbar \omega - E_g - E_0^{(d)} }}{{E_0 }}} \right)^{(d - 2)/2} \sum\limits_k {\Theta (\hbar \omega - E_g - E_0^{(d)} )A(\omega )} </math>

			The application of this result to semiconductor is important to understand the optical measurement data and the electronic properties. Some example shows the negative absorption coefficient that is fundamental presentation of [[Laser diode\|semiconductor laser]].

			==References==
			1. H. Haug and S. W. Koch, "[http://books.google.co.kr/books?id=-UoG0Hx0w04C&dq=Quantum+Theory+of+the+Optical+and+Electronic+Properties+of+Semiconductors&printsec=frontcover&source=bn&hl=ko&ei=DoneSeT7Ipne7APqv6AJ&sa=X&oi=book_result&ct=result&resnum=5 Quantum Theory of the Optical and Electronic Properties of Semiconductors]
			", World Scientific (1994). sec.5.4 a

			[[Category:Quantum mechanics]]

en>JuanFox: /* Safety effects of road geometry */

2012-08-13T01:42:17Z

Safety effects of road geometry

New page

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