Quantum yield - Revision history

en>SzMithrandir: format

2014-11-24T14:21:14Z

format

← Older revision		Revision as of 16:21, 24 November 2014
Line 1:		Line 1:
	~~[[Image:Pseudorapidity_plot.svg\|thumb\|right\|Pseudorapidity values shown on a polar plot. In [[particle physics]], an angle of zero~~ is ~~usually along the beam axis,~~ and ~~thus particles with high pseudorapidity values are generally lost, escaping through the space in the detector along with the beam~~.]]		Jayson Berryhill is how I'm called and my wife doesn't like it at all. It's not a common thing but what she likes doing is to perform domino but she doesn't have the time lately. Distributing production is how he tends to make a residing. Her family members life in Ohio.<br><br>Also visit my homepage ... psychic readings online; [http://www.edmposts.com/build-a-beautiful-organic-garden-using-these-ideas/ www.edmposts.com],
	~~[[Image:Pseudorapidity2.png\|thumb\|right\|As angle increases from zero, pseudorapidity decreases from infinity.]]~~
	~~In experimental [[particle physics]],~~ '~~''pseudorapidity''', <math>\eta</math>, is a commonly used spatial [[coordinate]] describing the angle of~~ a ~~particle relative to the beam axis. It is defined as~~
	~~:<math>\eta = -\ln\left[\tan\left(\frac{\theta}{2}\right)\right],</math>~~
	where <math>\theta </math> is the angle between the particle momentum <math>\mathbf{p}</math> and the beam axis.<ref>Introduction to High-Energy Heavy-Ion Collisions, by [[Cheuk-Yin Wong]], See page 24 for definition of rapidity.</ref> Inversely,
	~~:<math>\theta = 2\tan^{-1}\left(e^{-\eta}\right).</math>~~
	~~In terms of the momentum, the pseudorapidity variable can be written as~~
	~~:<math>\eta = \frac{1}{2} \ln \left(\frac{\left\|\mathbf{p}\right\|+p_\text{L}}{\left\|\mathbf{p}\right\|-p_\text{L}}\right),</math>~~
	~~where <math>p_\text{L}</math> is the component of the momentum along the beam axis. In the limit where the particle~~ is ~~travelling close~~ to ~~the speed of light, or in the approximation that the mass of the particle is nearly zero, pseudorapidity is numerically close to the experimental particle physicist~~'~~s definition of rapidity,~~
	~~:<math>y = \frac{1}{2} \ln \left(\frac{E+p_\text{L}}{E-p_\text{L}}\right)</math>~~
	~~This differs slightly from~~ the ~~definition of [[rapidity]] in [[special relativity]], which uses <math>\left\|\mathbf{p}\right\|</math> instead of <math>p_\text{L}</math>~~. ~~However, pseudorapidity depends only on the polar angle of its trajectory, and not on the energy of the particle.~~

	~~In hadron collider physics, the rapidity (or pseudorapidity) is preferred over the polar angle <math>\theta</math> because, loosely speaking, particle~~ production is ~~constant as~~ a ~~function of rapidity~~. ~~One speaks of the "forward" direction~~ in ~~a hadron collider experiment, which refers to regions of the detector that are close to the beam axis, at high <math>\|\eta\|~~.<~~/math>~~

	~~The rapidity as a function of pseudorapidity is given by~~
	~~:<math~~>~~y = \ln \frac{\sqrt{m^2 + p_T^2 \cosh^2 \eta} + p_T \sinh \eta}{\sqrt{m^2 + p_T^2}}.~~<~~/math~~>
	~~The difference in the rapidity of two particles is independent of [[Lorentz boost]]s along the beam axis.~~

	~~== Values ==~~
	~~[[Image:Pseudorapidity~~.~~svg\|thumb\|right\|300px\|A plot of polar angle vs~~. ~~pseudorapidity~~.]]

	~~Here are some representative values~~:
	~~:{\| class=wikitable~~
	~~! <math>\theta</math>~~
	~~! <math>\eta</math>~~
	~~! <math>\theta<~~/~~math>~~
	~~! <math>\eta<~~/~~math>~~
	\|-
	~~\| 0°~~
	~~\| ∞~~
	~~\| 180°~~
	~~\| −∞~~
	\|-
	~~\| 0~~.1°
	~~\| 7~~.04
	~~\| 179.9°~~
	~~\| −7.04~~
	\|-
	~~\| 0.5°~~
	~~\| 5.43~~
	~~\| 179.5°~~
	~~\| −5.43~~
	\|-
	~~\| 1°~~
	~~\| 4.74~~
	~~\| 179°~~
	~~\| −4.74~~
	\|-
	~~\| 2°~~
	~~\| 4.05~~
	~~\| 178°~~
	~~\| −4.05~~
	\|-
	~~\| 5°~~
	~~\| 3.13~~
	~~\| 175°~~
	~~\| −3.13~~
	\|-
	~~\| 10°~~
	~~\| 2.44~~
	~~\| 170°~~
	~~\| −2.44~~
	\|-
	~~\| 20°~~
	~~\| 1.74~~
	~~\| 160°~~
	~~\| −1.74~~
	\|-
	~~\| 30°~~
	~~\| 1.32~~
	~~\| 150°~~
	~~\| −1.32~~
	\|-
	~~\| 45°~~
	~~\| 0.88~~
	~~\| 135°~~
	~~\| −0.88~~
	\|-
	~~\| 60°~~
	~~\| 0.55~~
	~~\| 120°~~
	~~\| −0.55~~
	\|-
	~~\| 80°~~
	~~\| 0.175~~
	~~\| 100°~~
	~~\| −0.175~~
	\|-
	~~\| 90°~~
	~~\| 0~~
	~~\|colspan=2\|~~
	\|}

	~~Pseudorapidity is odd about <math>\theta = 90<~~/~~math> degrees~~. ~~In other words, <math>\eta(\theta)=-\eta(180^\circ-\theta)</math>~~.

	~~==Conversion to Cartesian Momenta==~~

	Hadron colliders measure physical momenta in terms of transverse momentum <math>p_\text{T}</math>, polar angle in the transverse plane <math>\phi</math> and pseudorapidity <math>\eta</math>. To obtain cartesian momenta <math>(p_x, p_y, p_z)</math> (with the <math>z</math>-axis defined as the beam axis), ~~the following conversions are used:~~
	~~:<math> p_x = p_\text{T} \cos \phi </math>~~
	~~:<math> p_y = p_\text{T} \sin \phi </math>~~
	~~:<math> p_z = p_\text{T} \sinh{\eta}</math>.~~

	~~Therefore, <math> \|p\|= p_\text{T} \cosh{\eta}</math>.~~

	~~==References==~~
	~~{{Reflist}}<!--added above categories/infobox footers by script-assisted edit-->~~

	~~[[Category:Particle physics]]~~

en>MrOllie: Reverted 1 edit by Spreus (talk): WP:EL. (TW)

2013-09-11T14:38:59Z

Reverted 1 edit by Spreus (talk): WP:EL. (TW)

← Older revision		Revision as of 16:38, 11 September 2013
Line 1:		Line 1:
	~~Hi there~~, ~~I am Sophia~~. ~~Since he was eighteen he~~'~~s been operating~~ as ~~an information officer but he plans on changing it~~. ~~Playing badminton~~ is ~~a factor~~ that he is ~~completely addicted~~ to~~. For many years she~~'s ~~been residing~~ in ~~Kentucky but her spouse desires them~~ to ~~move~~.<br><br>~~My web blog~~ ... ~~[http~~://~~koreanyelp~~.~~com~~/~~index~~.~~php?document_srl~~=~~1798&mid~~=~~SchoolNews telephone psychic~~]		[[Image:Pseudorapidity_plot.svg\|thumb\|right\|Pseudorapidity values shown on a polar plot. In [[particle physics]], an angle of zero is usually along the beam axis, and thus particles with high pseudorapidity values are generally lost, escaping through the space in the detector along with the beam.]]
			[[Image:Pseudorapidity2.png\|thumb\|right\|As angle increases from zero, pseudorapidity decreases from infinity.]]
			In experimental [[particle physics]], '''pseudorapidity''', <math>\eta</math>, is a commonly used spatial [[coordinate]] describing the angle of a particle relative to the beam axis. It is defined as
			:<math>\eta = -\ln\left[\tan\left(\frac{\theta}{2}\right)\right],</math>
			where <math>\theta </math> is the angle between the particle momentum <math>\mathbf{p}</math> and the beam axis.<ref>Introduction to High-Energy Heavy-Ion Collisions, by [[Cheuk-Yin Wong]], See page 24 for definition of rapidity.</ref> Inversely,
			:<math>\theta = 2\tan^{-1}\left(e^{-\eta}\right).</math>
			In terms of the momentum, the pseudorapidity variable can be written as
			:<math>\eta = \frac{1}{2} \ln \left(\frac{\left\|\mathbf{p}\right\|+p_\text{L}}{\left\|\mathbf{p}\right\|-p_\text{L}}\right),</math>
			where <math>p_\text{L}</math> is the component of the momentum along the beam axis. In the limit where the particle is travelling close to the speed of light, or in the approximation that the mass of the particle is nearly zero, pseudorapidity is numerically close to the experimental particle physicist's definition of rapidity,
			:<math>y = \frac{1}{2} \ln \left(\frac{E+p_\text{L}}{E-p_\text{L}}\right)</math>
			This differs slightly from the definition of [[rapidity]] in [[special relativity]], which uses <math>\left\|\mathbf{p}\right\|</math> instead of <math>p_\text{L}</math>. However, pseudorapidity depends only on the polar angle of its trajectory, and not on the energy of the particle.

			In hadron collider physics, the rapidity (or pseudorapidity) is preferred over the polar angle <math>\theta</math> because, loosely speaking, particle production is constant as a function of rapidity. One speaks of the "forward" direction in a hadron collider experiment, which refers to regions of the detector that are close to the beam axis, at high <math>\|\eta\|.</math>

			The rapidity as a function of pseudorapidity is given by
			:<math>y = \ln \frac{\sqrt{m^2 + p_T^2 \cosh^2 \eta} + p_T \sinh \eta}{\sqrt{m^2 + p_T^2}}.</math>
			The difference in the rapidity of two particles is independent of [[Lorentz boost]]s along the beam axis.

			== Values ==
			[[Image:Pseudorapidity.svg\|thumb\|right\|300px\|A plot of polar angle vs. pseudorapidity.]]

			Here are some representative values:
			:{\| class=wikitable
			! <math>\theta</math>
			! <math>\eta</math>
			! <math>\theta</math>
			! <math>\eta</math>
			\|-
			\| 0°
			\| ∞
			\| 180°
			\| −∞
			\|-
			\| 0.1°
			\| 7.04
			\| 179.9°
			\| −7.04
			\|-
			\| 0.5°
			\| 5.43
			\| 179.5°
			\| −5.43
			\|-
			\| 1°
			\| 4.74
			\| 179°
			\| −4.74
			\|-
			\| 2°
			\| 4.05
			\| 178°
			\| −4.05
			\|-
			\| 5°
			\| 3.13
			\| 175°
			\| −3.13
			\|-
			\| 10°
			\| 2.44
			\| 170°
			\| −2.44
			\|-
			\| 20°
			\| 1.74
			\| 160°
			\| −1.74
			\|-
			\| 30°
			\| 1.32
			\| 150°
			\| −1.32
			\|-
			\| 45°
			\| 0.88
			\| 135°
			\| −0.88
			\|-
			\| 60°
			\| 0.55
			\| 120°
			\| −0.55
			\|-
			\| 80°
			\| 0.175
			\| 100°
			\| −0.175
			\|-
			\| 90°
			\| 0
			\|colspan=2\|
			\|}

			Pseudorapidity is odd about <math>\theta = 90</math> degrees. In other words, <math>\eta(\theta)=-\eta(180^\circ-\theta)</math>.

			==Conversion to Cartesian Momenta==

			Hadron colliders measure physical momenta in terms of transverse momentum <math>p_\text{T}</math>, polar angle in the transverse plane <math>\phi</math> and pseudorapidity <math>\eta</math>. To obtain cartesian momenta <math>(p_x, p_y, p_z)</math> (with the <math>z</math>-axis defined as the beam axis), the following conversions are used:
			:<math> p_x = p_\text{T} \cos \phi </math>
			:<math> p_y = p_\text{T} \sin \phi </math>
			:<math> p_z = p_\text{T} \sinh{\eta}</math>.

			Therefore, <math> \|p\|= p_\text{T} \cosh{\eta}</math>.

			==References==
			{{Reflist}}<!--added above categories/infobox footers by script-assisted edit-->

			[[Category:Particle physics]]

en>My very best wishes: /* Examples */ this needs to be reorganized but not removed

2012-07-08T05:05:39Z

Examples: this needs to be reorganized but not removed

New page

Hi there, I am Sophia. Since he was eighteen he's been operating as an information officer but he plans on changing it. Playing badminton is a factor that he is completely addicted to. For many years she's been residing in Kentucky but her spouse desires them to move.<br><br>My web blog ... [http://koreanyelp.com/index.php?document_srl=1798&mid=SchoolNews telephone psychic]

← Older revision		Revision as of 16:21, 24 November 2014
Line 1:		Line 1:
	~~[[Image:Pseudorapidity_plot.svg\|thumb\|right\|Pseudorapidity values shown on a polar plot. In [[particle physics]], an angle of zero~~ is ~~usually along the beam axis,~~ and ~~thus particles with high pseudorapidity values are generally lost, escaping through the space in the detector along with the beam~~.]]		Jayson Berryhill is how I'm called and my wife doesn't like it at all. It's not a common thing but what she likes doing is to perform domino but she doesn't have the time lately. Distributing production is how he tends to make a residing. Her family members life in Ohio.<br><br>Also visit my homepage ... psychic readings online; [http://www.edmposts.com/build-a-beautiful-organic-garden-using-these-ideas/ www.edmposts.com],
	~~[[Image:Pseudorapidity2.png\|thumb\|right\|As angle increases from zero, pseudorapidity decreases from infinity.]]~~
	~~In experimental [[particle physics]],~~ '~~''pseudorapidity''', <math>\eta</math>, is a commonly used spatial [[coordinate]] describing the angle of~~ a ~~particle relative to the beam axis. It is defined as~~
	~~:<math>\eta = -\ln\left[\tan\left(\frac{\theta}{2}\right)\right],</math>~~
	where <math>\theta </math> is the angle between the particle momentum <math>\mathbf{p}</math> and the beam axis.<ref>Introduction to High-Energy Heavy-Ion Collisions, by [[Cheuk-Yin Wong]], See page 24 for definition of rapidity.</ref> Inversely,
	~~:<math>\theta = 2\tan^{-1}\left(e^{-\eta}\right).</math>~~
	~~In terms of the momentum, the pseudorapidity variable can be written as~~
	~~:<math>\eta = \frac{1}{2} \ln \left(\frac{\left\|\mathbf{p}\right\|+p_\text{L}}{\left\|\mathbf{p}\right\|-p_\text{L}}\right),</math>~~
	~~where <math>p_\text{L}</math> is the component of the momentum along the beam axis. In the limit where the particle~~ is ~~travelling close~~ to ~~the speed of light, or in the approximation that the mass of the particle is nearly zero, pseudorapidity is numerically close to the experimental particle physicist~~'~~s definition of rapidity,~~
	~~:<math>y = \frac{1}{2} \ln \left(\frac{E+p_\text{L}}{E-p_\text{L}}\right)</math>~~
	~~This differs slightly from~~ the ~~definition of [[rapidity]] in [[special relativity]], which uses <math>\left\|\mathbf{p}\right\|</math> instead of <math>p_\text{L}</math>~~. ~~However, pseudorapidity depends only on the polar angle of its trajectory, and not on the energy of the particle.~~

	~~In hadron collider physics, the rapidity (or pseudorapidity) is preferred over the polar angle <math>\theta</math> because, loosely speaking, particle~~ production is ~~constant as~~ a ~~function of rapidity~~. ~~One speaks of the "forward" direction~~ in ~~a hadron collider experiment, which refers to regions of the detector that are close to the beam axis, at high <math>\|\eta\|~~.<~~/math>~~

	~~The rapidity as a function of pseudorapidity is given by~~
	~~:<math~~>~~y = \ln \frac{\sqrt{m^2 + p_T^2 \cosh^2 \eta} + p_T \sinh \eta}{\sqrt{m^2 + p_T^2}}.~~<~~/math~~>
	~~The difference in the rapidity of two particles is independent of [[Lorentz boost]]s along the beam axis.~~

	~~== Values ==~~
	~~[[Image:Pseudorapidity~~.~~svg\|thumb\|right\|300px\|A plot of polar angle vs~~. ~~pseudorapidity~~.]]

	~~Here are some representative values~~:
	~~:{\| class=wikitable~~
	~~! <math>\theta</math>~~
	~~! <math>\eta</math>~~
	~~! <math>\theta<~~/~~math>~~
	~~! <math>\eta<~~/~~math>~~
	\|-
	~~\| 0°~~
	~~\| ∞~~
	~~\| 180°~~
	~~\| −∞~~
	\|-
	~~\| 0~~.1°
	~~\| 7~~.04
	~~\| 179.9°~~
	~~\| −7.04~~
	\|-
	~~\| 0.5°~~
	~~\| 5.43~~
	~~\| 179.5°~~
	~~\| −5.43~~
	\|-
	~~\| 1°~~
	~~\| 4.74~~
	~~\| 179°~~
	~~\| −4.74~~
	\|-
	~~\| 2°~~
	~~\| 4.05~~
	~~\| 178°~~
	~~\| −4.05~~
	\|-
	~~\| 5°~~
	~~\| 3.13~~
	~~\| 175°~~
	~~\| −3.13~~
	\|-
	~~\| 10°~~
	~~\| 2.44~~
	~~\| 170°~~
	~~\| −2.44~~
	\|-
	~~\| 20°~~
	~~\| 1.74~~
	~~\| 160°~~
	~~\| −1.74~~
	\|-
	~~\| 30°~~
	~~\| 1.32~~
	~~\| 150°~~
	~~\| −1.32~~
	\|-
	~~\| 45°~~
	~~\| 0.88~~
	~~\| 135°~~
	~~\| −0.88~~
	\|-
	~~\| 60°~~
	~~\| 0.55~~
	~~\| 120°~~
	~~\| −0.55~~
	\|-
	~~\| 80°~~
	~~\| 0.175~~
	~~\| 100°~~
	~~\| −0.175~~
	\|-
	~~\| 90°~~
	~~\| 0~~
	~~\|colspan=2\|~~
	\|}

	~~Pseudorapidity is odd about <math>\theta = 90<~~/~~math> degrees~~. ~~In other words, <math>\eta(\theta)=-\eta(180^\circ-\theta)</math>~~.

	~~==Conversion to Cartesian Momenta==~~

	Hadron colliders measure physical momenta in terms of transverse momentum <math>p_\text{T}</math>, polar angle in the transverse plane <math>\phi</math> and pseudorapidity <math>\eta</math>. To obtain cartesian momenta <math>(p_x, p_y, p_z)</math> (with the <math>z</math>-axis defined as the beam axis), ~~the following conversions are used:~~
	~~:<math> p_x = p_\text{T} \cos \phi </math>~~
	~~:<math> p_y = p_\text{T} \sin \phi </math>~~
	~~:<math> p_z = p_\text{T} \sinh{\eta}</math>.~~

	~~Therefore, <math> \|p\|= p_\text{T} \cosh{\eta}</math>.~~

	~~==References==~~
	~~{{Reflist}}<!--added above categories/infobox footers by script-assisted edit-->~~

	~~[[Category:Particle physics]]~~