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{{Image|Planar Schottky diode.PNG|right|250px|Planar Schottky diode with ''n<sup>+</sup>''-guard rings and tapered oxide.}}
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==Schottky diode==
==Coordinate system==
The '''Schottky diode''' is a two-terminal device consisting of conductive ''gate'' (for example, a metal) on top of a semiconductor ''body''. A generic name for this structure is the '''metal-semiconductor diode''' or '''M/S diode'''.<ref name=Sah>


The term "Schottky diode" may be taken erroneously to refer to diffusion as the mechanism of operation as first proposed by Mott, Schottky and Davydov. However, the mechanism in most devices is [[thermionic emission]], as later proposed by Bethe. See {{cite book |title= Fundamentals of solid-state electronics |author=Chih-Tang Sah |url=http://books.google.com/books?id=205wsYbl2fAC&pg=PA474 |pages=p. 474 |chapter=§560: Metal/semiconductor diode |isbn=9810206372 |year=1991 |publisher=World Scientific}}
The coordinates of a point '''r''' in an ''n''-dimensional real numerical space ℝ<sup>n</sup> or a complex ''n''-space ℂ<sup>n</sup>  are simply an ordered set of ''n'' real or complex numbers:<ref name=Korn>


</ref> For low voltage applications, below 200V, silicon is used, but for higher voltages (up to 3000 V or more) silicon carbide is used to extend the breakdown voltage. These voltages are achievable only when edge breakdown is avoided, which requires special attention to ''edge termination'' designs.<ref name=Baliga>
{{cite book |title=Mathematical handbook for scientists and engineers : definitions, theorems, and formulas for reference and review |author=Granino Arthur Korn, Theresa M. Korn |pages=p. 169 |url=http://books.google.com/books?id=xHNd5zCXt-EC&pg=PA169&dq=curvilinear+%22coordinate+system%22&lr=&as_brr=0&sig=ACfU3U3psSqwpBtA3U40e46VPPaMNMEw4g#PPA169,M1
|isbn=0486411478 |year=2000 |publisher=Courier Dover Publications}}


{{cite book |chapter= §3.2 Schottky diode edge terminations |title=Silicon carbide power devices |author=B. Jayant Baliga |year=2005 |isbn=9812566058 |publisher=World Scientific |url=http://books.google.com/books?id=LNLVwAzhN7EC&pg=PA44 |pages=pp. 44 ''ff''}}
</ref><ref name=Morita>[http://books.google.com/books?id=5N33Of2RzjsC&pg=PA12&dq=geometry++axiom+%22coordinate+system%22&lr=&as_brr=0&sig=ACfU3U3Vi7xsLiYiWCK0erF6X2gczHOkJA#v=onepage&q&f=false Morita]
</ref><ref name=Fritzche>


</ref> The figure shows three strategies toward increasing the edge breakdown voltage: an extension of the metal diode contact over a tapered oxide and also an ''n<sup>+</sup>''-guard ring and a floating guard ring. These strategies are sometimes used together, but also are used separately. The substrate contact is made through an ''ohmic contact'' to the ''p''-substrate made using a metal-to-''p<sup>+</sup>'' region on the surface of the diode.
[http://books.google.com/books?id=jSeRz36zXIMC&pg=PA155&dq=complex+%22coordinate+system%22&hl=en&ei=LA2JTYD1MYfWtQP2j92NDA&sa=X&oi=book_result&ct=result&resnum=1&ved=0CCkQ6AEwAA#v=onepage&q=complex%20%22coordinate%20system%22&f=false Fritzche]</ref>
:<math>\mathbf{r} =[x^1,\ x^2,\ \dots\ ,  x^n] \ .</math>
Coordinate surfaces, coordinate lines, and [[Basis (linear algebra)|basis vectors]] are components of a '''coordinate system'''.<ref name=Zdunkowski>{{cite book |title=Dynamics of the Atmosphere |page=84  |isbn=052100666X |year=2003 |author=Wilford Zdunkowski & Andreas Bott |publisher=Cambridge University Press |url=http://books.google.com/books?id=GuYvC21v3g8C&pg=RA1-PA84&dq=%22curvilinear+coordinate+system%22&lr=&as_brr=0&sig=ACfU3U2g2k7kY5u-CVcJ1pH5ZxsbEb9Rig  }}</ref>


==Applications==
==Manifolds==
The Schottky diode is used in a large variety of applications, ranging from practical devices for switching, rectification and photo-detection, to test structures for fabrication monitoring and for studies of semiconductor defects and processes.
A coordinate system in mathematics is a facet of [[geometry]] or of [[algebra]], in particular, a property of [[Manifold (geometry)|manifold]]s (for example, in physics, [[configuration space]]s or [[phase space]]s).<ref name=Hawking>


==Operation==
According to Hawking and Ellis: "A manifold is a space locally similar to Euclidean space in that it can be covered by coordinate patches. This structure allows differentiation to be defined, but does not distinguish between different coordinate systems. Thus, the only concepts defined by the manifold structure are those that are independent of the choice of a coordinate system." {{cite book |title=The Large Scale Structure of Space-Time |author=Stephen W. Hawking & George Francis Rayner Ellis |isbn=0521099064 |year=1973 |publisher=Cambridge University Press |pages=p. 11 |url=http://books.google.com/books?id=QagG_KI7Ll8C&pg=PA59&dq=manifold+%22The+Large+Scale+Structure+of+Space-Time%22&lr=&as_brr=0&sig=ACfU3U1q-iaRTBDo6J8HMEsyPeFi8cJNWg#PPA11,M1
Three different bias cases are examined: zero bias, forward bias, and reverse bias. A simplified one dimensional analysis along a line vertically through the center of the Schottky contact is used throughout. It is imagined that the ''p<sup>+</sup>''-ohmic contact is vertically below the Schottky contact.
}} A mathematical definition is: ''A connected [[Hausdorff space]] ''M'' is called an ''n''-dimensional manifold if each point of ''M'' is contained in an open set that is homeomorphic to an open set in Euclidean ''n''-dimensional space.''
{{Image|Schottky barrier height.PNG|right|250px|Schottky barrier formation on ''p''-type semiconductor. Energies are in eV.}}
====Zero bias====
The figure shows (top) a charge-neutral, partly filled metal energy band and a charge-neutral semiconductor valence and conduction band, electrically isolated from each other. The Fermi level in the ''p''-type semiconductor is near its valence band edge, as set by its acceptor impurity doping. (See [[Fermi function#Fermi level|Fermi level]]). The Fermi level in the metal marks the top of the filled electron energy levels in a partly filled band of the metal.  


Ordinarily, the Fermi levels of different materials differ. When they are brought into electrical contact, enabling electron transfer between the materials, the work done in removing an electron from one material and placing it in the other is equal to the energy difference in the Fermi levels. Consequently, energy is released upon contact by electron transference from the material with the higher Fermi level to the material with the lower Fermi level. This charge transfer continues until the electrical charge difference means the energy gain from transfer is countered by the electrical work required against the charge difference. At this point the two Fermi levels are brought into coincidence and no further charge transfer occurs. This flat Fermi level situation (bottom panel) corresponds to [[thermal equilibrium]], and no net current flows once equilibrium is reached.  
</ref><ref name=Morita2>
{{cite book |title=Geometry of Differential Forms |author=Shigeyuki Morita, Teruko Nagase, Katsumi Nomizu |pages=p. 12 |url=http://books.google.com/books?id=5N33Of2RzjsC&pg=PA12&dq=geometry++axiom+%22coordinate+system%22&lr=&as_brr=0&sig=ACfU3U3Vi7xsLiYiWCK0erF6X2gczHOkJA#PPA12,M1
|isbn=0821810456 |year=2001 |publisher=American Mathematical Society Bookstore }}


The occurrence of charge transfer naturally means that the two materials acquire a charge. In the figure, the metal loses electrons and forms an extremely thin positive charge layer near the interface. The semiconductor gains electrons, as indicated by the bending of the valence band edge away from the Fermi level, which increases the valence band occupancy by electrons. Differently stated, the vacancies (holes) in the valence band are reduced in number, and the charge balance in the band-bending region is lost. In this ''depletion layer'' (the holes or ''majority carriers'' are depleted), the immobile negative acceptor dopant ions make this region charge negative, and this charge results in a potential according to [[Maxwell equations#Poisson's equation|Poisson's equation]]. The potential decreases with distance toward the bulk semiconductor, and at some distance (the ''depletion width'') the bulk properties of the semiconductor are regained and the semiconductor bulk is charge neutral.
</ref> The coordinates of a point '''r''' in an ''n''-dimensional space are simply an ordered set of ''n'' numbers:<ref name=Korn>


The resulting potential drop across the semiconductor depletion layer is called the ''Schottky barrier height'', labeled ''&phi;<sub>B</sub>'' in the figure. It is a form of [[contact potential]].
{{cite book |title=Mathematical handbook for scientists and engineers : definitions, theorems, and formulas for reference and review |author=Granino Arthur Korn, Theresa M. Korn |pages=p. 169 |url=http://books.google.com/books?id=xHNd5zCXt-EC&pg=PA169&dq=curvilinear+%22coordinate+system%22&lr=&as_brr=0&sig=ACfU3U3psSqwpBtA3U40e46VPPaMNMEw4g#PPA169,M1
|isbn=0486411478 |year=2000 |publisher=Courier Dover Publications}}


{{Image|Schottky barrier (forward bias).PNG|right|250px|Under forward bias ''V<sub>F</sub>'' the Schottky barrier height is reduced and the Fermi levels are split.}}
</ref>
:<math>\mathbf{r} =[x^1,\ x^2,\ \dots\ ,  x^n] \ .</math>


====Forward bias====
In a general [[Banach space]], these numbers could be (for example) coefficients in a functional expansion like a [[Fourier series]]. In a physical problem, they could be [[spacetime]] coordinates or [[normal mode]] amplitudes. In a [[Robotics|robot design]], they could be angles of relative rotations, linear displacements, or deformations of [[linkage (mechanical)|joints]].<ref name=Yamane>
If a forward bias voltage is applied ''V<sub>F</sub>'', the Fermi level of the bulk metal ''E<sub>Fm</sub>'' (in eV) is raised in energy above the bulk Fermi level in the semiconductor ''E<sub>Fp</sub>'', which lowers the Schottky barrier height to a value ''&phi;<sub>B</sub>−V<sub>F</sub>''. A current of holes now flows from the semiconductor to the metal (or, equivalently, of electrons from the metal to the semiconductor). Notice that the alignment of the metal Fermi level relative to the semiconductor band edges is not changed by the bias: that is fixed by the processes involved in adjusting the Fermi levels to achieve equilibrium at zero applied bias.


A current flows under forward bias. According to the model of [[thermionic emission]], the electron current flowing toward the semiconductor is proportional to the electron density at the metal side of the interface, while the electron current flowing toward the metal is proportional to the electron density at the semiconductor side. At zero bias there is no current, but under forward bias the electron density on the metal side is unaffected, while that on the semiconductor side is reduced by the forward bias. Translating the matter to the terminology of holes, and using a simple [[Fermi_function#Boltzmann_limit|Boltzmann approximation]] to the [[Fermi function]], the hole density on the semiconductor side is increased by a factor:
{{cite book |author=Katsu Yamane |title=Simulating and Generating Motions of Human Figures |isbn=3540203176 |year=2004 |publisher=Springer  |pages=12–13 |url=http://books.google.com/books?id=tNrMiIx3fToC&pg=PA12&dq=generalized+coordinates+%22kinematic+chain%22&lr=&as_brr=0&sig=ACfU3U3LRGJJTAHs21CHdOvuu08vw0cAuw#PPA13,M1  }}


:<math> p(V_F) = p(0)e^{qV_F/k_BT} \ , </math>
</ref> Here we will suppose these coordinates can be related to a [[Cartesian coordinate]] system by a set of functions:
:<math>x^j = x^j (x,\  y,\  z,\  \dots)\ , </math>&ensp; &ensp; <math> j = 1, \ \dots \ , \ n\  </math>


where ''p(0)'' is the zero forward bias value of hole density on the semiconductor side. The hole current from the semiconductor to the metal therefore is increased by this factor. The current, being by convention a flow of positive charge, is therefore positive from the semiconductor to the metal, and the Schottky barrier current in forward bias becomes:
where ''x'', ''y'', ''z'', ''etc.'' are the ''n'' Cartesian coordinates of the point. Given these functions, '''coordinate surfaces''' are defined by the relations:


:<math>I(V_F) = I(0)\left( e^{qV_F/k_BT}-1 \right) \ . </math>
:<math> x^j (x, y, z, \dots) = \mathrm{constant}\ , </math>&ensp; &ensp; <math> j = 1, \ \dots \ , \ n\  .</math>


Due to some complications of real Schottky barriers, the current is usually represented as:
The intersection of these surfaces define '''coordinate lines'''. At any selected point, tangents to the intersecting coordinate lines at that point define a set of '''basis vectors''' {'''e'''<sub>1</sub>, '''e'''<sub>2</sub>, …, '''e'''<sub>n</sub>} at that point. That is:


:<math>I(V_F) = I(0)\left( e^{qV_F/nk_BT}-1 \right) \ , </math>
:<math>\mathbf{e}_i(\mathbf{r}) =\lim_{\epsilon \rightarrow 0} \frac{\mathbf{r}\left(x^1,\  \dots,\  x^i+\epsilon,\  \dots ,\  x^n \right) - \mathbf{r}\left(x^1,\  \dots,\  x^i,\  \dots ,\  x^n \right)}{\epsilon }\ ,</math>


where the factor ''n'' is usually larger than one and is called the ''ideality factor''.
which can be normalized to be of unit length. For more detail see [[curvilinear coordinates]].


{{Image|Schottky barrier (reverse bias).PNG|right|250px|Schottky diode under reverse bias ''V<sub>R</sub>''.}}
Coordinate surfaces, coordinate lines, and [[Basis (linear algebra)|basis vectors]] are components of a '''coordinate system'''.<ref name=Zdunkowski>{{cite book |title=Dynamics of the Atmosphere |page=84  |isbn=052100666X |year=2003 |author=Wilford Zdunkowski & Andreas Bott |publisher=Cambridge University Press |url=http://books.google.com/books?id=GuYvC21v3g8C&pg=RA1-PA84&dq=%22curvilinear+coordinate+system%22&lr=&as_brr=0&sig=ACfU3U2g2k7kY5u-CVcJ1pH5ZxsbEb9Rig  }}</ref> If the basis vectors are orthogonal at every point, the coordinate system is an [[Orthogonal coordinates|orthogonal coordinate system]].


====Reverse bias====
An important aspect of a coordinate system is its [[Metric (mathematics)|metric]] ''g''<sub>ik</sub>, which determines the [[arc length]] ''ds'' in the coordinate system in terms of its coordinates:<ref name=Borisenko>{{cite book |title=Vector and Tensor Analysis with Applications |author= A. I. Borisenko, I. E. Tarapov, Richard A. Silverman |page=86 |url=http://books.google.com/books?id=CRIjIx2ac6AC&pg=PA86&dq=coordinate+metric&lr=&as_brr=0&sig=ACfU3U1osXaT2hg7Md57cJ9katl3ttL43Q
If a reverse bias ''V<sub>R</sub>'' is applied, the Fermi level of the metal is lowered below that of the semiconductor, and the barrier height for holes is increased on the semiconductor side by the amount of the reverse bias. The hole density is therefore decreased compared to equilibrium (the electron occupancy increases) and the current from the semiconductor falls below the equilibrium value. That means the diode current changes direction compared to the forward biased case.
|isbn=0486638332 |publisher=Courier Dover Publications |year=1979 |pages=pp. 86 ''ff'' |chapter=§2.8.4 Arc length. Metric coefficients |edition=Reprint of Prentice-Hall 1968 ed  }}</ref>


==Notes==
:<math>(ds)^2 = g_{ik}\ dx^i\ dx^k \ , </math>
<references/>
http://books.google.com/books?id=LNLVwAzhN7EC&pg=PA45&dq=%22Schottky+diode%22&hl=en&ei=iAg6TeO7AYSasAOk67WhAw&sa=X&oi=book_result&ct=result&resnum=9&ved=0CGcQ6AEwCA#v=onepage&q=%22Schottky%20diode%22&f=false


http://books.google.com/books?id=FPlJQ0iO7oQC&pg=PA134&dq="Schottky+diode"&hl=en&ei=iAg6TeO7AYSasAOk67WhAw&sa=X&oi=book_result&ct=result&resnum=8&ved=0CGIQ6AEwBw#v=onepage&q="Schottky diode"&f=false
where repeated indices are summed over.


http://books.google.com/books?id=sh94bLWOTY4C&pg=PA84&dq=%22Schottky+diode%22&hl=en&ei=iAg6TeO7AYSasAOk67WhAw&sa=X&oi=book_result&ct=result&resnum=1&ved=0CDwQ6AEwAA#v=onepage&q=%22Schottky%20diode%22&f=false
As is apparent from these remarks, a coordinate system is a mathematical construct, part of an [[axiomatic system]]. There is no necessary connection between coordinate systems and physical motion (or any other aspect of reality). However, coordinate systems can be used to describe motion by interpreting one coordinate as time. Thus, [[Lorentz transformation]]s and [[Galilean transformation]]s may be viewed as [[coordinate transformation]]s.


http://books.google.com/books?id=GTM2i6ZFpIEC&pg=PA299&dq=%22Schottky+diode%22&hl=en&ei=Afc6TZXzL5G6sQPaoYidAw&sa=X&oi=book_result&ct=result&resnum=1&ved=0CDIQ6AEwADgK#v=onepage&q=%22Schottky%20diode%22&f=false


http://books.google.com/books?id=pRFUZdHb688C&pg=PA245&dq=%22Schottky+diode%22&hl=en&ei=Afc6TZXzL5G6sQPaoYidAw&sa=X&oi=book_result&ct=result&resnum=4&ved=0CEMQ6AEwAzgK#v=onepage&q=%22Schottky%20diode%22&f=false
==Notes==
 
<references/>
http://books.google.com/books?id=7WKOfUR-8M4C&pg=PA227&dq=%22Schottky+diode%22&hl=en&ei=tvg6TbqyCIjQsAOTsbTVAw&sa=X&oi=book_result&ct=result&resnum=1&ved=0CDAQ6AEwADgU#v=onepage&q=%22Schottky%20diode%22&f=false
[http://books.google.com/books?id=hUWEXphqLo8C&pg=PA111&dq=manifold+%22coordinate+system%22&hl=en&ei=I5GGTbWsPIz2tgOmoIzoAQ&sa=X&oi=book_result&ct=result&resnum=5&ved=0CEQQ6AEwBA#v=onepage&q=manifold%20%22coordinate%20system%22&f=false Choquet-Bruhat]
 
[http://books.google.com/books?id=sRaSuentwngC&pg=PA2&dq=manifold+%22coordinate+system%22&hl=en&ei=I5GGTbWsPIz2tgOmoIzoAQ&sa=X&oi=book_result&ct=result&resnum=2&ved=0CDIQ6AEwAQ#v=onepage&q=manifold%20%22coordinate%20system%22&f=false Bishop]
http://books.google.com/books?id=XrSI2C9NlDIC&pg=PA47&dq=%22Schottky+diode%22&hl=en&ei=tvg6TbqyCIjQsAOTsbTVAw&sa=X&oi=book_result&ct=result&resnum=9&ved=0CFwQ6AEwCDgU#v=onepage&q=%22Schottky%20diode%22&f=false
[http://books.google.com/books?id=CGk1eRSjFIIC&pg=PA3&dq=manifold+%22coordinate+system%22&hl=en&ei=I5GGTbWsPIz2tgOmoIzoAQ&sa=X&oi=book_result&ct=result&resnum=7&ved=0CE8Q6AEwBg#v=onepage&q=manifold%20%22coordinate%20system%22&f=false O'Neill]
 
[http://books.google.com/books?id=iaeUqc2yQVQC&pg=PA31&dq=manifold+%22coordinate+system%22&hl=en&ei=I5GGTbWsPIz2tgOmoIzoAQ&sa=X&oi=book_result&ct=result&resnum=9&ved=0CFgQ6AEwCA#v=onepage&q=manifold%20%22coordinate%20system%22&f=false Warner]
http://books.google.com/books?id=REQkwBF4cVoC&pg=PA599&dq=%22Schottky+diode%22&hl=en&ei=YQM7TedHjsSwA-Tj4fwC&sa=X&oi=book_result&ct=result&resnum=3&ved=0CEAQ6AEwAjge#v=onepage&q=%22Schottky%20diode%22&f=false
 
http://onlinelibrary.wiley.com/doi/10.1002/1521-4095%2820020605%2914:11%3C789::AID-ADMA789%3E3.0.CO;2-H/pdf
 
http://books.google.com/books?id=iMSnDxI7JNsC&pg=PA181&dq=%22Schottky+diode%22&hl=en&ei=wkg7TdJ-jKKwA96_3IsD&sa=X&oi=book_result&ct=result&resnum=8&ved=0CFkQ6AEwBzgy#v=onepage&q=%22Schottky%20diode%22&f=false
 
http://books.google.com/books?id=LNLVwAzhN7EC&pg=PA50&dq=%22guard+ring%22+%22edge+termination%22&hl=en&ei=7ks7TeGTMI-ssAPipv3ZAw&sa=X&oi=book_result&ct=result&resnum=3&ved=0CEYQ6AEwAg#v=onepage&q=%22guard%20ring%22%20%22edge%20termination%22&f=false
 
[http://books.google.com/books?id=pMxTrOQtIw8C&pg=PA381&dq=edge+termination+breakdown&hl=en&ei=hoA7TauKNpDAsAOHsZS6Aw&sa=X&oi=book_result&ct=result&resnum=3&ved=0CDEQ6AEwAg#v=onepage&q=edge%20termination%20breakdown&f=false Compare pn diode and Schottky diode for speed and breakdown]

Latest revision as of 11:20, 14 September 2024


The account of this former contributor was not re-activated after the server upgrade of March 2022.


Coordinate system

The coordinates of a point r in an n-dimensional real numerical space ℝn or a complex n-space ℂn are simply an ordered set of n real or complex numbers:[1][2][3]

Coordinate surfaces, coordinate lines, and basis vectors are components of a coordinate system.[4]

Manifolds

A coordinate system in mathematics is a facet of geometry or of algebra, in particular, a property of manifolds (for example, in physics, configuration spaces or phase spaces).[5][6] The coordinates of a point r in an n-dimensional space are simply an ordered set of n numbers:[1]

In a general Banach space, these numbers could be (for example) coefficients in a functional expansion like a Fourier series. In a physical problem, they could be spacetime coordinates or normal mode amplitudes. In a robot design, they could be angles of relative rotations, linear displacements, or deformations of joints.[7] Here we will suppose these coordinates can be related to a Cartesian coordinate system by a set of functions:

   

where x, y, z, etc. are the n Cartesian coordinates of the point. Given these functions, coordinate surfaces are defined by the relations:

   

The intersection of these surfaces define coordinate lines. At any selected point, tangents to the intersecting coordinate lines at that point define a set of basis vectors {e1, e2, …, en} at that point. That is:

which can be normalized to be of unit length. For more detail see curvilinear coordinates.

Coordinate surfaces, coordinate lines, and basis vectors are components of a coordinate system.[4] If the basis vectors are orthogonal at every point, the coordinate system is an orthogonal coordinate system.

An important aspect of a coordinate system is its metric gik, which determines the arc length ds in the coordinate system in terms of its coordinates:[8]

where repeated indices are summed over.

As is apparent from these remarks, a coordinate system is a mathematical construct, part of an axiomatic system. There is no necessary connection between coordinate systems and physical motion (or any other aspect of reality). However, coordinate systems can be used to describe motion by interpreting one coordinate as time. Thus, Lorentz transformations and Galilean transformations may be viewed as coordinate transformations.


Notes

  1. 1.0 1.1 Granino Arthur Korn, Theresa M. Korn (2000). Mathematical handbook for scientists and engineers : definitions, theorems, and formulas for reference and review. Courier Dover Publications, p. 169. ISBN 0486411478. 
  2. Morita
  3. Fritzche
  4. 4.0 4.1 Wilford Zdunkowski & Andreas Bott (2003). Dynamics of the Atmosphere. Cambridge University Press. ISBN 052100666X. 
  5. According to Hawking and Ellis: "A manifold is a space locally similar to Euclidean space in that it can be covered by coordinate patches. This structure allows differentiation to be defined, but does not distinguish between different coordinate systems. Thus, the only concepts defined by the manifold structure are those that are independent of the choice of a coordinate system." Stephen W. Hawking & George Francis Rayner Ellis (1973). The Large Scale Structure of Space-Time. Cambridge University Press, p. 11. ISBN 0521099064.  A mathematical definition is: A connected Hausdorff space M is called an n-dimensional manifold if each point of M is contained in an open set that is homeomorphic to an open set in Euclidean n-dimensional space.
  6. Shigeyuki Morita, Teruko Nagase, Katsumi Nomizu (2001). Geometry of Differential Forms. American Mathematical Society Bookstore, p. 12. ISBN 0821810456. 
  7. Katsu Yamane (2004). Simulating and Generating Motions of Human Figures. Springer, 12–13. ISBN 3540203176. 
  8. A. I. Borisenko, I. E. Tarapov, Richard A. Silverman (1979). “§2.8.4 Arc length. Metric coefficients”, Vector and Tensor Analysis with Applications, Reprint of Prentice-Hall 1968 ed. Courier Dover Publications, pp. 86 ff. ISBN 0486638332. 

Choquet-Bruhat Bishop O'Neill Warner