新加坡F1夜賽

轉錄自林帛亨--賽車與生活:新加坡F1夜賽
Published: 中國賽車誌 10月出版 Option改裝車雜誌11月出版 (台灣)

剛結束的新加坡F1大獎賽 只有一個形容詞  “夢幻” Hanss我在現場看F1也好幾個年頭  說實話 看到後來 連有人贊助機票 酒店到現場看都覺得意興闌珊

或者就算在現場比F1墊賽 比賽結束後也沒啥興趣看  說真的大部分比賽現場只能看到一兩個彎道 唯一能看到就是不停重複一樣的畫面  煞車 降檔 轉彎 幸運點看個輪胎冒煙 試圖超車就很好了 但這樣的畫面重複再重複的看  沒兩年就真的很膩
這兩年來因為在ESPN StarSport當賽車講評 所以都看電視的直播居多 看久了總覺得賽道雖然不同  但整個感覺了無新意 但看到了新加坡夜賽後 我想賽車就該是這樣 為什麼一定要很熱的大太陽下比賽呢 對觀眾對車手車隊都是折磨
---新加坡大獎賽將成為全球街賽的典範

[Tennis] ATP World Tour Final Portraits 2008-2012, 2014

World tour final 2014 London O2

Staying up on 'Trends'

From: http://www.atpworldtour.com/Media/Photo-Landing.aspx


World tour final 2013 London... still searching for a good photo here...

World tour final 2012 London

The Origin of Species - Charles Darwin

Originally titled On the Origin of Species by Means of Natural Selection, or the Preservation of Favored Races in the Struggle for Life, this landmark work was first published in November of 1859.

Formula 1

Aerodynamic simulation

Citation needed: BMW Sauber F1 Team?

Scientific WorkPlace 5.0

How to change the space between floats and captions

Version: 2.x, 3.x, 4.x, 5.x - Scientific WorkPlace and Scientific Word

From http://www.mackichan.com

LaTeX defines the space above and below the captions of floating objects (both graphics and tables) with the macros\abovecaptionskip and \belowcaptionskip. Many typesetting specifications use these macros, including sebase.cls, which defines each value as 10 pt.

Although the Style Editor doesn't provide a method for changing these values, you can alter the space between floating objects and their captions. You can add an external macro that is associated with the typesetting specifications for your document. Alternatively, you can change the spacing for all floating objects in a document by modifying the document preamble, or you can change the spacing for an individual floating object by placing TeX commands before and after the object.

周杰倫 & 林志玲

Supershells

Supershells are periodic modulations in the amplitude of quantal shell structure
From http://fy.chalmers.se/~klavs/supershells.htm
Here is the physics behind it, briefly and applied to metal clusters. Clusters are approximately spherical and the valence electrons have a 2(2L+1) degeneracy associated with each set of quantum numbers (n,L)=(number of radial nodes, angular momentum). These are the subshells. Different values of (n,L) tend to bunch into groups. These groups are called shells (and not supershells, as some people will have it). This bunching is actually a more common phenomenon than usually thought. The perodic table is an example of this shell structure, although it is not quite as simple to understand as metal clusters.

The bunching of subshells into shells can be understood in terms of semiclassical physics. Technically, the density of states at the Fermi level can be calculated as a sum over closed classical trajectories (orbits). The modulation of the density of states with energy is an equivalent manifestation of shell structure. Apart from a constant term, the most important classical trajectories are the trianglesand the squares. The appearance of the triangles and squares can be understood in a simpler way (see Bohr and Mottelson's book Nuclear Structure). 
The shell structure induced by triangular orbits have a certain period in energy. The density of states varies periodically when you go up in energy from the bottom of the Fermi sea to the Fermi level and beyond. This periodicity can be converted into a periodic variation of the stability of clusters with size. The variations occur linearly with the radius of the cluster, and consequently linearly with the cuberoot of the number of atoms, N, in the cluster (for a metal of constant density).

This explains the fact that shell closings, as observed in mass abundance spectra and in the ionization energies, are spaced with a constant increment in the cuberoot of N. If one tries to calculate what the spacing in N^1/3 actually is, it turns out that it depends on what closed orbit you are looking at. The triangles give one period and the square orbits give another. But these are approximately equally important in metal clusters (for realistic shapes of the single particle potential etc.). This means that there is a beating pattern between the triangular and square orbits. This is the supershell.
The average shell period in N^1/3 for triangles and squares is about 0.6. The difference is small, about 10% of the mean value. So the result is that you see electronic shells with a spacing of approximately 0.6 with an amplitude which is modulated with a much longer period. The modulation is periodic with N^1/3. The first node appears around N=1000 (with the Woods-Saxon potential), or N=800 in more realistic calculations (LDA).

The term supershell is well chosen: supershells are the periodic modulation in amplitude of a periodic modulation of the stability/density of states (the shells). The word 'super' doesn't mean 'something you are supposed to be impressed by'. Here is a definition: super- pref. 1) Above; over; upon: 2) More inclusive than a specified category: superorder.

Some history of supershells in metal clusters
The phenomenon found it's way into cluster science when a group of nuclear physicists, led by Sven Bjørnholm at the Bohr institute in Copenhagen embarked on a study of metal clusters, around 1987. The enterprise was inspired by the close similarities between the valence electrons in metal clusters, in particular the simple metals such as the alkalis, and the also fermionic nucleons in nuclei. The first project of the group was to use this analogy in persuit of the shell structure which had been discovered by W.D.Knight and his group in Berkeley in 1984. The ideas and the machinery which can be found in Bohr and Mottelson's Nuclear Structure were applied to metal clusters, and we managed to both predict and observe the supershells. Happily other researchers also saw the supershells later, both in theory and in experiments, and not just in sodium clusters, but in a number of other metals. More recently the supershells have been observed in the quantized conductance of small junctions in low temperature experiments!

References:
The prediction of supershell: Supershells in metal clusters, H.Nishioka, K.Hansen and B.R.Mottelson, Phys.Rev. B 42 (1990) 9377.
The experiment of supershell: Observation of quantum supershells in clusters of sodium atoms, J.Pedersen, S.Bjørnholm, J.Borggreen, K.Hansen, T.P.Martin and H.D.Rasmussen: Nature 353 (1991) 733.