{"title":"算术电路的阈值实现","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":"{\"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}","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
摘要
如果R不完全等于Ri,会有什么影响?如果L-COMPARATOR U out ItCES TO中的R比Ri大,则电路表现出惯常的LL / uu / uu +9x>C_~ \ 4°/ >跃迁,在upp > 0时发生跃迁,在y ~ 8w时交替发生跃迁。ui,,uo的UH->UL转换[图6(c)]。自理想图1-理想比较器特性。条件[图6(b)]包含在这些图5中。隧道的复合特性(简化)在两种情况下,可以精确地获得二极管具有电特性ple的原理二极管对。在实际应用中,与图3所示类似的微小迟滞量。当然,这是不可避免的。R对于高速运行,不受迟滞影响取决于二极管结ca
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-