{"title":"Threshold Realization of Arithmetic Circuits","authors":"M. Fischler, E. Poe","doi":"10.1109/TEC.1962.5219366","DOIUrl":null,"url":null,"abstract":"uout t What is the effect if R is not made and maintained exactly equal to Ri? If R is larger a in L-COMPARATOR U out ItCES TO than Ri then the circuit exhibits customary LL| UH <E HIGH STATE H \\ f.& 4 hysteresis [Fig. 6(a) ]. In this case, the UL-*>UI H\\ e+9x>C_~ \\ 4°/ > transition occurs for uip>uo, and alternately au s iY~08 w . the UH->UL transition for ui,,<uo. Conversely, '0v SWITCHES TO uf R is smaller than Ri, the situation is reversed LOW STATEu U L (S~'+ u) -u'~+ u2) so that UL--5U1 takes place for uiX<uo and --UL (uc' +ut) <.//(u'^+u2) -*UL for uii>uo [Fig. 6(c)]. Since the ideal Fig. 1-Ideal comparator characteristic. condition [Fig. 6(b)] is embraced by these Fig. 5-Composite characteristic (simplified) of a tunneltwo cases, it can be attained exactly in princidiode pair whose diodes have electrical characteristics ple. In practice, a minute amount of hysteresis similar to those shown in Fig. 3. is, of course, inevitable. ;R For high-speed operation, freedom from hysteresis will depend on diode junction ca-","PeriodicalId":177496,"journal":{"name":"IRE Trans. Electron. Comput.","volume":"10 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1962-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"7","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"IRE Trans. Electron. Comput.","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/TEC.1962.5219366","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 7
Abstract
uout t What is the effect if R is not made and maintained exactly equal to Ri? If R is larger a in L-COMPARATOR U out ItCES TO than Ri then the circuit exhibits customary LL| UH UI H\ e+9x>C_~ \ 4°/ > transition occurs for uip>uo, and alternately au s iY~08 w . the UH->UL transition for ui,,uo [Fig. 6(c)]. Since the ideal Fig. 1-Ideal comparator characteristic. condition [Fig. 6(b)] is embraced by these Fig. 5-Composite characteristic (simplified) of a tunneltwo cases, it can be attained exactly in princidiode pair whose diodes have electrical characteristics ple. In practice, a minute amount of hysteresis similar to those shown in Fig. 3. is, of course, inevitable. ;R For high-speed operation, freedom from hysteresis will depend on diode junction ca-