This message is in MIME format. Since your mail reader does not understand this format, some or all of this message may not be legible. ------_=_NextPart_000_01BF6327.14F8F900 Content-Type: text/plain; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable Dear Quanbo, This effect has been examined mainly during the 1970s when gold interconnection lines were still in wider use. In short: Chromium is = not soluble in bulk Au but it is soluble in Au grain boundaries. Cr will = thus diffuse through the thin film grain boundaries and so increase their resistance. Since a grain boundary may extend over the whole width of a metal runner, a small amount of Cr can cause a large increase of the = runner resistance. You may have observed that this resistance is not constant = over short periods of time (seconds) but readily varies by 10...100%. On the surface, Cr is oxidised and as an oxide will not travel back, so after some time, all the Cr has accumulated on the surface. The = adhesion layer has then disappeared and eventually the high resistance of the metallization will return to its original value (nearly). Hope to have helped you; for literature see among others: * Munitz, A.; Komem, Y.: Structural and resistivity changes in = heat-treated chromium-gold films. In: Thin Solid Films 37 (1976) , pp. 171-179. * Gupta, D.; Ho, P.S. : Diffusion Processes in Thin Films. In: Thin = Solid Films 72 (1980) , pp. 399-418. * Richards, J.L.; McCann, W.H.: Low Temperature Diffusion in = Polycrystalline Thin-Film Gold-Nickel Couples. In: Journal of Vacuum Science and = Technology (1969) , pp. 644-647. * Hieber, H.: Aging Properties of Gold Layers with Different Adhesion Layers. In: Thin Solid Films 37 (1976) , pp. 335-343. * Holloway, P.H.; Amos, D.E.; Nelson, G.C.: Analysis of grain-boundary diffusion in thin films: Chromium in gold. In: Journal of Applied = Physics 47 (1976) , 9 , pp. 3769-3775. * Audino, R.; Gestefanis, G.: Interface Behaviour Evaluation in Au/Cr, = Au/Ti and Au/Pd/Ti Thin Films by Means of Resistivity and Stylus = Measurements. In: Thin Solid Films 36 (1976) , pp. 343-347. * Munitz, A.; Komem, Y.: The Increase in the Electrical Resistance of Heat-Treated Au/Cr Films. In: Thin Solid Films 71 (1980) , pp. 177-188. * Yan, B.; Lin, T.; Mao, D.; Yang, C.: Interdiffusion of an Au/Ni/Cr multilayer metallization on silicon substrates. In: Thin Solid Films = 173 (1989) , pp. 39-51. * George, M.A.; Glaunsinger, W.S.; Thundat, T; Lindsay, S.M.: = Electrical, Spectroscopic, and Morphological Investigation of Chromium Diffusion = Through Gold Films. In: Thin Solid Films 189 (1990) , S. 59-72. Yours sincerely, Kai Hiltmann Kai Hiltmann, HSG-IMIT, Wilhelm-Schickard-Str. 10, D-78052 Villingen-Schwenningen, Germany Ext. ++49-7721-943-132, Fax ++49-7721-943-140 -----Urspr=FCngliche Nachricht----- Von: Zou Quanbo [mailto:Quanbo@ime.org.sg] Gesendet am: Montag, 27. Dezember 1999 03:23 An: MEMS@ISI.EDU Betreff: Cr/Au thermal-electric property Dear all, I experienced that the electric resistivity of Cr/Au bi-layer thin-film resistor was drastically increased after a thermal treatment. The = process condition was: rough vacuum (~Torr), 380 degC, 2 hours. Cr/Au (thickness=3D1k/3k angstroms) are on Pyrex substrate (sputtered on). = The resulted resistivity was ~20 times higher than un-treated samples. Does any one know what happened to this? I appreciate if somebody can = help explain and maybe solve this problem. Thanks and best regards, Merry X'mas and Happy New Year! Quanbo Zou =3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D= =3D=3D=3D=3D=3D=3D=3D=3D=3D Dr. Quanbo Zou MEMS Department Institute of Microelectronics 11 Science Park Road Singapore Science Park II Singapore 117685 Tel: 65-7705905(O) 65-2642113(H) Fax: 65-7731915 Email: quanbo@ime.org.sg =3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D= =3D=3D=3D=3D=3D=3D=3D=3D =20 ------_=_NextPart_000_01BF6327.14F8F900 Content-Type: application/ms-tnef Content-Transfer-Encoding: base64 eJ8+IjMJAQaQCAAEAAAAAAABAAEAAQeQBgAIAAAA5AQAAAAAAADoAAEIgAcAGAAAAElQTS5NaWNy b3NvZnQgTWFpbC5Ob3RlADEIAQWAAwAOAAAA0AcBABQACgAQADEABAA7AQEggAMADgAAANAHAQAU AAoAEAAxAAQAOwEBCYABACEAAAA5Mzk5NDZDQkU2Q0REMzExQThCNTAwNTAwNDQ2NTFDMgAGBwEE gAEAJAAAAEFXOiBDci9BdSB0aGVybWFsLWVsZWN0cmljIHByb3BlcnR5ALYMAQ2ABAACAAAAAgAC AAEDkAYA7BAAADYAAAACATEAAQAAABwBAABQQ0RGRUIwOQABAAIAZwAAAAAAAAA4obsQBeUQGqG7 CAArKlbCAABFTVNNREIuRExMAAAAAAAAAAAbVfogqmYRzZvIAKoAL8RaDAAAAElNSVRFWAAvbz1I U0cvb3U9SU1JVC9jbj1SZWNpcGllbnRzL2NuPUthaQAuAAAAAAAAAKM5BxC/X9MRqKMAUARGUcIB ADElirtAWtMRqJUAUARGUcIAAAAB5NEAAAAAAAAuAAAAAAAAAKM5BxC/X9MRqKMAUARGUcIBADEl irtAWtMRqJUAUARGUcIAAAAB9AUAABAAAACTmUbL5s3TEai1AFAERlHCJAAAAEFXOiBDci9BdSB0 aGVybWFsLWVsZWN0cmljIHByb3BlcnR5AAMA3j+vbwAAAwA2AAAAAAADAAWACCAGAAAAAADAAAAA AAAARgAAAABShQAA8BMAAB4AJYAIIAYAAAAAAMAAAAAAAABGAAAAAFSFAAABAAAABAAAADguNQAL ANaACCAGAAAAAADAAAAAAAAARgAAAAAGhQAAAAAAAAMAJoAIIAYAAAAAAMAAAAAAAABGAAAAAAGF AAAAAAAACwAAgAggBgAAAAAAwAAAAAAAAEYAAAAAA4UAAAAAAAALAC+ACCAGAAAAAADAAAAAAAAA RgAAAAAOhQAAAAAAAAMAAoAIIAYAAAAAAMAAAAAAAABGAAAAABCFAAAAAAAAAwAwgAggBgAAAAAA wAAAAAAAAEYAAAAAEYUAAAAAAAADADKACCAGAAAAAADAAAAAAAAARgAAAAAYhQAAAAAAAB4AQYAI IAYAAAAAAMAAAAAAAABGAAAAADaFAAABAAAAAQAAAAAAAAAeAEKACCAGAAAAAADAAAAAAAAARgAA AAA3hQAAAQAAAAEAAAAAAAAAHgBDgAggBgAAAAAAwAAAAAAAAEYAAAAAOIUAAAEAAAABAAAAAAAA AAsAx4ALIAYAAAAAAMAAAAAAAABGAAAAAACIAAAAAAAACwDJgAsgBgAAAAAAwAAAAAAAAEYAAAAA BYgAAAAAAAACAQkQAQAAAPgJAAD0CQAA6A8AAExaRnUV4YnhAwAKAHJjcGcxMjXiMgNDdGV4BUEB AwH3TwqAAqQD4wIAY2gKwHPwZXQwIAcTAoAP8wBQfwRWCFUHshHFDlEDARDHMvcGAAbDEcUzBEYQ yRLbEdPbCO8J9zsYvw4wNRHCDGDOYwBQCwkBZDM2EVALpyJjATAgRGUKwVF1OwBwBuAsCqIKhAqA VGh9BAAgAREFkAVAEPAEIGJjCeEfkHhhbQuACYAgQwDAC4BseSBkCHFuAGcgdGhlIDE5tDcwBCB3 IiADoGcG8NchEAuADrByBaBuIPAf4PJpAiAgbCDhIpEEkCIwunMkAGwDIAuAIqBpBIFEIHURIC4g SQOgcypoGGE6EsBoA2FpdaZtI0AEIG5vBUBzBvAOdQJgIjAlYWJ1bGvtEWB1KIEFQGkpMQQgJ+mf KOEJwAtxIEAIYG5kCsD1CJBzJiBDBcAD8CUxIhB3JfAhkAaQZiXxIgEDYHXcZ2giAyIQJWFmAxAn UP0qniAAcCEQJ+AjQQUAHeD5LNNlaQXAGMAAkCUAAHDaYyYRUy/hIjBhLlwhgJ8AwCGADsEJ8CEQ b3YTIX8iEiKwBvA0ISWgIhAzoGZvMeEHgAGQAyByKxAg8HL6LDHhcwDAJTEgwCsBBUD7NQErsWMD kTeALMIx8Atg/HJnKEIwBTUBIhI1tDDLvlkIYDLzEPAzwDOgYhEg7nIzwCEQIhBhBUAtwQQgfzDY J2YjoTESNwEzwiZzID5wBnEEcAQgOTIHcSAo9xEgI6E/gCkpAzARLIAhcYp2LxRiIYAxMC5CUNFC MDAlLh6UTwOgIhLqcwhwZgDQZTYQK7EfcfxveCWgBAAhAS9yICEDke9EkjSCJTEnonQqoDPAAyDa YgDQazYQL7FhAYA+ov8DcCzhB3E2ESwDIjArsSAS/QDQYydAKKA8UCEBJCFDafcmIB9QMdFkIiAA kCQiMxCfEyEgEiIRA6BEwWFwPzD7CsBE9WUzwAIwHjAlMCGAfyISH2AtUTzZOTU1UyRQer88UCQS K+MYwE5wBKF0L8H2dD+RBRBnC4A1gUGQCkFvQCAg8ArAIXApQsUelEjebz8wUiI7UyIgbD8wIRD6 eQhgOy4ABbEkUCNxPFD/CHAk4QngNqIh4SewIiARELo6HpoqBdArEClQejYQVEEuVlBLSCFtNhBZ +i4mwFNGsBtwUeE1gS9y+TDUaXYpUCGAEOEh4AeR9yVhIiA8UC1GsF0xIQEQ4P0nBC0jAy4SK4Em QCbAH1FNA6BTBvAloCBGXuIg7DM3QCAiUTZAsDYQTXChJiAxNzEtYZA5QsWpWTBHdQUwYTYQRFnh Y1TgNhBQLlMmICbARPsskyQSUANgMVAEEFzEX4OfYDNfL2A0AcBgsjgwYRaAMzk5LTQxOGIHHlIN 4BDxP4A2EEouTFFZ4U1jQwBwbjYQV6QuSFqRTG8H4FRaQK8/MVcEY/glYVAG8HkFAN55MRFQ0SDw ZlMtYDJigOkjES1ODeBrRvEIUQtQuytyZiJKCGFS8jUBVgDQ8nUnQVNjCJAxsy+Ba5A3EOAnoBhQ ZyGAYME2OaFhFjY0NC1zsDdiB95ICJAgUDYBaxJBUtEh8P9kkT8xJAAHkTUBbsJrQExSvyKRKVAt YGPyJME28UFLxg93BGYPYD9oJDM1LTPcNDN0KAbwGFB3MxBjYrtrEFZQQQRgaeFjAEVZ4Y0HwGwn 4GrBRy5DdULfUvFtgERiNRAqky0ydyyEv2y1LcdYUCbZIuRv/0FNcNMkUCEBUGh/oWMEIHQAPWC4 OWgGYPBokGCQNzVfYgco4CyAJ6A2EFJZ4Uf/B5AOsEPQAwBp4X8AJsAmQOMjcUPSIEJlO1EkEAhw 3CBFUzJRFCozLyuwWbHPjAAHYC9ji/FQZIyCZWjdQfJNHeAGMTUBUlvJL3L9WsB5CkAEII5xQ6Fa QE5R+3lPelY2eu18EHvxdBhZX79aZEtyJkAwBYGzIjBFKDC/H+AFEDeAAyCPBE/WSF0y3lRdhYvz Za9muzFnnGGQajdhwDho2FkAcDYQQq1Z4UwLgDYQVGpCYWNR+2MCndFnRBGJpoEYNQKL0/9vEJnS SfElEUxTUJwkIQCQ/yRQI6FDkTuwRrEOsJpfelUdYZAzZ5NzJ2hhLTUxnWIIZQWwOHA2EE0uWdL+ RwtgKxAAkFyhNgFq8GOg91ZQH1ArEnSekZ5DP4B9Iv9joKjQJsCXWKuRPzCXgX3gXQWgcA3gNhEv gU0FsHC/NFFyoJezJkAzwCUBZ6M1/zcxJvZj+B9QLSR2s5ofparbpsBgsjln42OhNWiQAcD/VBs6 0XdBqYExUBjAIXA2EP5LC3B0oaIgA4ELkB6ptuoBdRFTRy1JTUlU/2rRAxBVsV5gcXAfYEdACxH3 ulBGsGFxMGLhtNBn0A5B/R6jViUhqZJuULphJLAjwK+8o37hBJADgXkelEUO0HEmICsrNLTBAcBh sDkRk7ExMzI2EEZheF2+/jQBQB6pHpQtwqJV4REQcHJcJxDQIeCj4f0iIU4A0CbwaYFdUMKivAWb AiAmwFo64R4kIFshMamiIG86HiRAB3EuqHHwLnNnXR6UiNEzcREwrzahJsCuAAIwYZ+xMnQQPR3B elpAdOEiQWiAIDB4MzoyFdAeo39gyPFFIQXgQElTSX4wRFWfHpSKcF1xASAmwXIvKOH7WBI2YS1G 8Jd0PyB15L5F7x6UHdM2cR6LSSCRPzJxoj88FyIwzjdbujcjzXJiafYtTEQtwi0uEh6UMNQFsf99 ECxhKqAlAZfBIXEv5kUB/0fDMfDNtUahXTGQ4ktUzsH/ZMIelEBiKVBRMyAgJsAtJCNBkHEjKH5U BbByKY02EDNn0CGQZWdDyXHfIAC14iuSzXEelCgtwUdAgSRxcz0xay8zKMA/XJGkcQNwQKFNoUpi UHnvGMDAUKRHQCFwKSAjcUpDf1QAS2LVx6IRIQFbutayfv8B0D/TBCBPIjPTA5ErEF1n701Qa7Bv ws9Lby9D0/Ft8f/fkGthIrA8URDwTXEg8lIx/TyCPyYwL2BNcBjAcYDiMvcGkEgDBuBkXFEDkVWy HpT/0XELYi9jMwEgUCfSO3E8g7vOwSghbVQbH1AAcGsvVP8gUCUAMMGvUGnCHpqOcN0Q2SGAWCcA wC9USE1hIYD1B8JZHeEhHprF1cWRHpT+Pfbv9+3Ppbsh9e7Loh3Bfwqx2ZPQ9T4RKVApIDkTTb8N 4ANgzjQCIIVxHpQxm+D9cXZQCsAowAgAQTAelDGRna9QcAWwIjD+S0lJ/15z/hBg8Dg1HvVG8CbA No974IdQu9C0IDUoT0CwHQNRMnOwv3C/4ChIKVfe5MAxAzUzIlAxApVF+8ZSJsBxxt72jwk/+LgO 8AUeo30LcB4AcAABAAAAIAAAAENyL0F1IHRoZXJtYWwtZWxlY3RyaWMgcHJvcGVydHkAAgFxAAEA AAAbAAAAAb9i7sDby0aWLc3mEdOotQBQBEZRwgANWAlgAAMAJgAAAAAAAwAuAAAAAAALACsAAAAA AAsAAgABAAAAHgBCEAEAAAAhAAAAPDEwMDAxMjAwMTI1LkFBMjAyMjRAazIuaXNpLmVkdT4AAAAA AwD9P+QEAABAADkAEOukFCdjvwEDAPE/BwQAAB4AMUABAAAABAAAAEtBSQADABpAAAAAAB4AMEAB AAAABAAAAEtBSQADABlAAAAAAAMAgBD/////CwDyEAEAAAACAUcAAQAAACsAAABjPURFO2E9IDtw PUhTRztsPUlNSVRFWC0wMDAxMjAwOTE2NDlaLTEyMzgAAAIB+T8BAAAAQAAAAAAAAADcp0DIwEIQ GrS5CAArL+GCAQAAAAAAAAAvTz1IU0cvT1U9SU1JVC9DTj1SRUNJUElFTlRTL0NOPUtBSQAeAPg/ AQAAAA0AAABLYWkgSGlsdG1hbm4AAAAAHgA4QAEAAAAEAAAAS0FJAAIB+z8BAAAAQAAAAAAAAADc p0DIwEIQGrS5CAArL+GCAQAAAAAAAAAvTz1IU0cvT1U9SU1JVC9DTj1SRUNJUElFTlRTL0NOPUtB SQAeAPo/AQAAAA0AAABLYWkgSGlsdG1hbm4AAAAAHgA5QAEAAAAEAAAAS0FJAEAABzDQpZUUJ2O/ AUAACDAA+fgUJ2O/AR4APQABAAAABQAAAEFXOiAAAAAAHgAdDgEAAAAgAAAAQ3IvQXUgdGhlcm1h bC1lbGVjdHJpYyBwcm9wZXJ0eQAeADUQAQAAAEYAAAA8MzEyNThBQkI0MDVBRDMxMUE4OTUwMDUw MDQ0NjUxQzIyQzA3MURAaW1pdGV4LmltaXQudW5pLXN0dXR0Z2FydC5kZT4AAAALACkAAQAAAAsA IwAAAAAAAwAGEKVRQDMDAAcQPAsAAAMAEBAAAAAAAwAREAAAAAAeAAgQAQAAAGUAAABERUFSUVVB TkJPLFRISVNFRkZFQ1RIQVNCRUVORVhBTUlORURNQUlOTFlEVVJJTkdUSEUxOTcwU1dIRU5HT0xE SU5URVJDT05ORUNUSU9OTElORVNXRVJFU1RJTExJTldJREVSAAAAAAIBfwABAAAARgAAADwzMTI1 OEFCQjQwNUFEMzExQTg5NTAwNTAwNDQ2NTFDMjJDMDcxREBpbWl0ZXguaW1pdC51bmktc3R1dHRn YXJ0LmRlPgAAAJLt ------_=_NextPart_000_01BF6327.14F8F900--