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Charge-Trapping Non-Volatile Memories: Volume 2--Emerging Materials and Structures PDF

215 Pages·2017·8.244 MB·English
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Panagiotis Dimitrakis E ditor Charge- Trapping Non-Volatile Memories Volume 2—Emerging Materials and Structures Charge-Trapping Non-Volatile Memories Panagiotis Dimitrakis Editor Charge-Trapping Non-Volatile Memories — Volume 2 Emerging Materials and Structures 123 Editor Panagiotis Dimitrakis Department ofMicroelectronics Institute of AdvancedMaterials Athens Greece ISBN978-3-319-48703-8 ISBN978-3-319-48705-2 (eBook) DOI 10.1007/978-3-319-48705-2 LibraryofCongressControlNumber:2016956818 ©SpringerInternationalPublishingAG2017 Thisworkissubjecttocopyright.AllrightsarereservedbythePublisher,whetherthewholeorpart of the material is concerned, specifically the rights of translation, reprinting, reuse of illustrations, recitation, broadcasting, reproduction on microfilms or in any other physical way, and transmission orinformationstorageandretrieval,electronicadaptation,computersoftware,orbysimilarordissimilar methodologynowknownorhereafterdeveloped. The use of general descriptive names, registered names, trademarks, service marks, etc. in this publicationdoesnotimply,evenintheabsenceofaspecificstatement,thatsuchnamesareexemptfrom therelevantprotectivelawsandregulationsandthereforefreeforgeneraluse. The publisher, the authors and the editors are safe to assume that the advice and information in this book are believed to be true and accurate at the date of publication. Neither the publisher nor the authorsortheeditorsgiveawarranty,expressorimplied,withrespecttothematerialcontainedhereinor foranyerrorsoromissionsthatmayhavebeenmade. Printedonacid-freepaper ThisSpringerimprintispublishedbySpringerNature TheregisteredcompanyisSpringerInternationalPublishingAG Theregisteredcompanyaddressis:Gewerbestrasse11,6330Cham,Switzerland Contents 1 Materials and Device Reliability in SONOS Memories... ..... .... 1 Krishnaswamy Ramkumar 2 Charge-Trap-Non-volatile Memory and Focus on Flexible Flash Memory Devices ... ..... .... .... .... .... .... ..... .... 55 Konstantina Saranti and Shashi Paul 3 Hybrid Memories Based on Redox Molecules.. .... .... ..... .... 91 Nikolaos Glezos 4 Organic Floating Gate Memory Structures.... .... .... ..... .... 123 S. Fakher, A. Sleiman, A. Ayesh, A. AL-Ghaferi, M.C. Petty, D. Zeze and Mohammed Mabrook 5 Nanoparticles-Based Flash-Like Nonvolatile Memories: Cluster Beam Synthesis of Metallic Nanoparticles and Challenges for the Overlying Control Oxide Layer.. ..... .... 157 E. Verrelli and D. Tsoukalas Index .... .... .... .... .... ..... .... .... .... .... .... ..... .... 211 v Chapter 1 Materials and Device Reliability in SONOS Memories Krishnaswamy Ramkumar 1.1 Introduction Non-volatile memories for data and code storage have been growing rapidly in performance and capacity over last few decades. With the advent of the many widely used consumer electronic gadgets such as cell phones, laptop computers, tablets, and electronic games, the need for non-volatile memories has been ever increasing recently. While the need for larger and larger memory capacity is obvious, there has also been an increasing demand for more and more robust data retention performance over a widening range of temperature. This is because the non-volatile memories are now getting into gadgets used in industrial and auto- motive environment. This coupled with the need for low cost solutions is chal- lenging the memory technology. SONOS (Silicon–Oxide–Nitride–Oxide–Silicon) seems to offer the non-volatile memory solutions in an ever widening range of applications.ThekeyfeaturesoftheSONOSmemorydeviceandtheirdependence on material characteristics are discussed in the following sections. 1.2 History of SONOS Memory Devices SONOS memory device has been known for many decades. The initial work on SONOSdeviceswasreportedinthelate1960s.TheMNS(Metal–Nitride–Silicon) structure was first proposed as an alternate to the MOS (Metal–Oxide–Silicon) K.Ramkumar(&) CypressSemiconductor,3833NorthFirstStreet,SanJose,USA e-mail:[email protected] ©SpringerInternationalPublishingAG2017 1 P.Dimitrakis(ed.),Charge-TrappingNon-VolatileMemories, DOI10.1007/978-3-319-48705-2_1 2 K.Ramkumar structureforsuperiordielectricstrength[1].However,instabilitieswerefoundwith this device due to the large density of interface states at the Nitride–Silicon inter- face.TheMNOS(Metal–Nitride–Oxide–Silicon)wasproposedasasolutiontothis instabilityonaccountofthestableinterfacebetweensilicondioxideandsilicon[2]. Thecharge storage intheMNOSstructurewasfirstobservedasahysteresisinthe threshold voltage as a function of the gate voltage as shown in Fig. 1.1 [3]. In these devices, the nitride layer was identified as the charge storage layer due tothetrapspresentandtheoxidelayerwasproposedforinjectingelectronsorholes by direct tunneling. These early MNOS devices were made using the Aluminum gatetechnologyTheMNOSconceptwasstudiedwidelyinthe1970sandappliedto memory structures [4–9]. With the advent of polysilicon gate technology, the AluminumwasreplacedbypolysiliconandSNOSdevicesbecameavailable.Inthe 1980s, to prevent carrier injection from the gate electrode to the nitride, another oxide layer was introduced between the nitride layer and the polysilicon gate and theSONOSdevicewasinvented[10].TheSONOStransistorwasthusconceivedas a storage element with its structure being almost identical to that of a MOS tran- sistor with the gate dielectric being replaced by a ONO dielectric. This device has beenstudiedextensivelyinthelastthreedecadestounderstandthecarriertransport, trappingandde-trappingmechanismsinthenitridelayer.Severalmechanismshave been proposed such as direct or modified Fowler–Nordiehm tunneling of carriers from the silicon to the nitride through the oxide and subsequent capture of these carriers by the deep traps in the nitride. The research on the SONOS device has continued with more sophisticated modeling of the transport and trapping mecha- nisms [11–13]. With the highlighting of the charge trapping mechanism in the SONOS device and its application in memories, the SONOS device also got referred to as a “Charge Trap Memory Device” or “CT” memory. Fig.1.1 Firstobservationof memoryeffectinMNOS device[3] 1 MaterialsandDeviceReliabilityinSONOSMemories 3 1.3 Floating Gate and SONOS Memories SONOS-based memories were first introduced in the 1980s with a 16 Kbit EEPROM as one of the first products. The competition at that time was from Floating gate memories. The different types of Floating gate transistors used in memories are shown in Fig. 1.2. In all cases, a conducting but electrically floating polysilicon layer is used for charge storage. ThesedevicesareusedeveninpresentdayFlash memorieswith device scaling beingthemaindriveroftheincreaseinmemorydensity.Manyenhancementssuch asMulti-levels andscaling havebeenintroduced intotheFloating gatetechnology to extend its capability. It is clear from the above figure that significant process changes are required to realize the floating gate memory device—a second polysiliconlayerdepositionandadditionalpatterningsteps.However,theretention performance of the Floating gate device is very robust on account of the relatively thick(60–80 Å)tunneloxidebeingused.ASONOSmemorydevice,ontheother hand, greatly resembles a regular MOSFET and requires very few changes to the basic MOS process. The only significant process change is the formation of the ONO dielectric which forms the gate dielectric of the SONOS device. A typical SONOS FET is shown in Fig. 1.3. The SONOS memories could not compete well against the Floating gate memories, in the 1980s because the program/erase voltages required to get sig- nificant tunneling currents were very high (>20 V) on account of the difficulty in scaling down the thicknesses of the layers of the ONO stack. With availability of better film deposition and metrology equipment subsequently, the ONO stack CG CG CG Float Float 14V SG Float e- Float SL SG FG FG FG S e- D S e- D S D Fig.1.2 Differentfloatinggatedeviceusedformemories Fig.1.3 Schematiccross sectionofatypicalSONOS FET Salicide Poly ONO Source Well Drain D-N Well 4 K.Ramkumar thicknesscouldbescaleddownwithrobustprocesscontrolandSONOSmemories capableofprogram/eraseatlowervoltageswereconceived.Additionally,extensive research on charge trap devices yielded novel methods of program and erase that allowed low voltage operation [14]. With this feature, SONOS memories became competitive with the floating gate memories and have carved a niche in the NVM market. The SONOS memory technology claims to be much less complex as compared to the Floating gate technology [15]. 1.4 SONOS Memory Devices As mentioned earlier, the simplest SONOS device closely resembles a normal CMOS FET (Fig. 1.4). The main difference isthat thegate dielectric now isa ONO dielectric made up of a tunnel oxide, a nitride and a blocking oxide. The transistor can be NMOS or PMOS and can be either enhancement type or depletion type. Depletion type has the benefit of a buried channel which keeps the carriers in the channel away from theinterfacestatesinTunneloxide–Semiconductorinterface.Ifthememorystackis described in more general terms, the three layers can be referred to as 1. The tunneling layer, used for injecting charge carriers into thetrap layer and to prevent trapped charges in the trap layer from being lost to the substrate. 2. The charge trap layer which stores charge by trapping the mobile carriers in traps located in the band gap. 3. The blocking layer which keeps the trapped charge in the trap layer isolated from the gate. N+ N+ P-Well Deep N-Well Poly Blocking Oxide (HTO) Nitride Tunnel Oxide Silicon Fig.1.4 ONOstackinaSONOSFET 1 MaterialsandDeviceReliabilityinSONOSMemories 5 All these are insulator layers which is a key difference from a floating gate memory device in which the charge storage layer is a semiconductor (Fig. 1.5). Infact, this difference gives a key advantage totheSONOSdevice. The charge carriersbeingtrappedinaninsulatormakesthemimmobilewhichmakesthedevice less susceptible to charge loss due to defects such as pin holes in contrast to a floating gate device where a defect can attract mobile charge carriers from every- where in the storage layer and give rise to a significant charge loss (Fig. 1.6). The three layers of the charge trap memory stack need not always be SiO and 2 SiN layers. For example, the tunneling layer can be a SiON layer or a high K Fig.1.5 DifferencesbetweenfloatinggateandSONOSmemorydevices[16] Fig.1.6 ComparisonofchargelossinfloatinggateandSONOSdevices

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