An Analytical Theory of Piezoresistive Effects in Hall Plates with Large Contacts

<div>Relative change of resistances of the equivalent resistor circuit (ERC) for offset-free (<svg height="14.8173pt" id="M573" style="vertical-align:-5.52897pt" version="1.1" viewbox="-0.0498162 -9.28833 51.8314 14.8173" width="51.8314pt" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink"><g transform="matrix(.013,0,0,-0.013,0,0)"><path d="M529 97L508 118C475 75 449 58 438 58C428 58 421 66 415 104C393 234 374 403 364 496C345 670 307 712 254 712C220 712 174 691 153 669L161 645C176 653 194 658 206 658C237 658 261 640 278 562C287 522 290 483 293 434C223 269 110 105 23 9L32 -12C59 -6 85 0 108 7C152 64 251 252 300 366C307 297 315 221 337 82C346 24 363 -12 393 -12C425 -12 475 13 529 97Z" id="g113-233"></path></g><g transform="matrix(.0091,0,0,-0.0091,7.761,3.132)"><path d="M620 667C620 684 593 710 552 710C515 710 459 687 409 634C360 582 334 506 320 433H247L215 400L220 388H310L259 80C224 -129 199 -161 185 -174C175 -183 160 -192 141 -192C123 -192 90 -181 75 -165C69 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Advances in Condensed Matter Physics

fig15

Figure 15

Figure 15: An Analytical Theory of Piezoresistive Effects in Hall Plates with Large Contacts 