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Prospects of Colloidal Nanocrystals for Electronic - Computer Science

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<strong>Colloidal</strong> <strong>Nanocrystals</strong> in <strong>Electronic</strong> Applications Chemical Reviews, 2010, Vol. 110, No. 1 441<br />

conventional flash memory is extremely prone to failure <strong>of</strong><br />

insulation; one weak spot in the tunneling oxide is sufficient<br />

to create a fatal discharge path (Figure 56d). A promising<br />

way to alleviate this problem, while still preserving the<br />

fundamental operation principles <strong>of</strong> the flash memory, is to<br />

store charge not on the continuous poly silicon FG, but on<br />

a layer <strong>of</strong> discrete, mutually isolated NCs (Figure 56b). Each<br />

NC will store only few electrons; collectively, the charges<br />

stored on NCs can control the threshold voltage <strong>of</strong> the FET.<br />

The concept <strong>of</strong> distributed charge storage is more faulttolerant<br />

because minor damages in the tunnel oxide layer<br />

are not detrimental <strong>for</strong> memory operation (Figure 56e).<br />

Thinner tunneling oxide can be used to achieve lower<br />

operating voltages and/or increase the operating speed.<br />

The properties <strong>of</strong> a thin SiO2 dielectric layer can be<br />

seriously degraded under continuous memory programming<br />

(write/erase), and this severely decreases the data retention<br />

time <strong>of</strong> conventional and NC-based flash memory devices.<br />

Stability increases with increasing oxide thickness; however,<br />

thicker oxide layer reduces the tunneling current through<br />

dielectric layer, requires higher operating voltages <strong>for</strong> write/<br />

erase, and puts restrictions on down-scaling dimensions <strong>of</strong><br />

the nodes. For most flash memories, the retention time and<br />

operating speed are in inverse proportion to each other.<br />

Several approaches have been studied to achieve the fast<br />

programming speed (write/erase) and the long retention time<br />

<strong>of</strong> memory simultaneously. 583-585 Recently, researchers have<br />

focused on improving data retention time without decreasing<br />

the programing speed at low voltages. 586-588 For this purpose,<br />

it was proposed to replace the conventional SiO2 dielectric<br />

layer with a high-k gate dielectric <strong>for</strong> the control and tunnel<br />

oxide layers. High-k dielectric materials with lower conduction<br />

band <strong>of</strong>fsets with Si provide lower tunneling barriers at<br />

the dielectric channel.<br />

The idea <strong>of</strong> NC-based flash memory has been proposed<br />

in 1996 by IBM. 571,582 Since then, different metal and<br />

semiconductor NCs have been tested as FGs. 589-592 The<br />

integration <strong>of</strong> 5 nm Si NCs into the gate oxide strongly<br />

affects the transfer characteristics <strong>of</strong> the MOSFET as shown<br />

in Figure 57. 593 In the control device where no FG is<br />

embedded into gate insulator, the drain current (ID) versus<br />

gate voltage (VG) scans show no hysteretic behavior; ID has<br />

same magnitude when VG is scanned from -4 to4Vand<br />

when VG is scanned from 4 to -4 V (Figure 57, dashed<br />

curve). However, huge hysteresis <strong>of</strong> transistor transfer<br />

characteristics is observed when small Si NCs are integrated<br />

into the gate oxide. For example, the difference in ID<br />

measured during <strong>for</strong>ward and backward gate scans exceeds<br />

10 6 at VG ) 0 V (Figure 57, solid curve). 593 Such behavior<br />

is fully consistent with flash memory operation principles<br />

described above; charging <strong>of</strong> NCs shifts the FET threshold<br />

voltage. The per<strong>for</strong>mance <strong>of</strong> NC flash memories depends<br />

strongly on the accurate control <strong>of</strong> NC size, density, and<br />

their uni<strong>for</strong>m distribution in a thin layer <strong>of</strong> oxide. 590,592,594,595<br />

Si and Ge Nanocrystal-Based Flash Memory Devices.<br />

Si NCs-based FG memory is seriously considered among<br />

the candidates <strong>for</strong> the next generation <strong>of</strong> nonvolatile memory<br />

devices. 370,571-573,584,596-604 Tiwari et al. reported the first Si<br />

NC-based FG memory device embedded in a SiO2 layer. 571<br />

The device operation is based on direct tunneling and storage<br />

<strong>of</strong> electrons in the NCs (also called nodes). Capacitance and<br />

size <strong>of</strong> the NCs limit the number <strong>of</strong> stored charges per node.<br />

Electron-injection occurs through direct tunneling from an<br />

inversion layer when positive (with respect to the source and<br />

Figure 57. Transfer characteristics (ID vs VG scan) <strong>of</strong> a nanocrystalbased<br />

flash memory device consisting <strong>of</strong> FET and the floating gate<br />

made <strong>of</strong> ∼5 nm Si nanocrystals separated from the transistor<br />

channel by a thin 9 nm layer <strong>of</strong> HfO2 tunnel oxide and from the<br />

control gate by a thicker layer (20 nm) <strong>of</strong> SiO2 control oxide. The<br />

presence <strong>of</strong> Si nanocrystals introduces hysteretic behavior <strong>of</strong> FET<br />

transter characteristics (solid line). The control experiment with<br />

same thicknesses <strong>of</strong> HfO2 and SiO2 layers but without Si nanocrystals<br />

shows nearly ideal transistor behavior with no hysteresis<br />

(dashed line). Reprinted with permission from ref 593. Copyright<br />

2006 American Institute <strong>of</strong> Physics.<br />

drain electrodes) gate voltage is applied (+VG). Such devices<br />

demonstrate high speed operation (less than 100s <strong>of</strong> nanosecond<br />

per write-erase cycle), small dimensions, and long<br />

operation times (excess <strong>of</strong> 10 9 cycles). 571 The per<strong>for</strong>mance<br />

<strong>of</strong> Si-based memories depends on the accurate control <strong>of</strong><br />

NC size, density, and arrangement in the thin oxide.<br />

Punchaipetch et al. studied the effect <strong>of</strong> tunnel layer<br />

thickness on the memory per<strong>for</strong>mance (write/erase) and data<br />

retention <strong>of</strong> Si NC-based floating gate devices. 605 The 10<br />

nm SiO2 tunnel oxide showed the most stable per<strong>for</strong>mance<br />

as compared to the 3 and 5 nm oxide layer. Degradation <strong>of</strong><br />

threshold voltage was not observed even after 10 8 operating<br />

cycles. Lu et al. reported the effect <strong>of</strong> NC density on the<br />

operation <strong>of</strong> the floating gate memory. 606 It was shown<br />

that the operating speed can be further increased by increasing<br />

the density <strong>of</strong> NCs in the FG layer. As mentioned above,<br />

the retention time is inversely correlated to the thickness <strong>of</strong><br />

the tunnel oxide layer.<br />

King et al. reported the gemanium NC memory devices<br />

that could operate at low voltages and high speeds superior<br />

to Si-based memory devices. 579 The device consisted <strong>of</strong><br />

MOSFET with Ge NC FGs embedded within the gate<br />

dielectric. Lu et al. also reported the memory devices with<br />

Ge NCs embedded in LaAlO3 (LAO) high-k dielectric. 607<br />

This device showed a significant memory effect with a very<br />

high density <strong>of</strong> stored charge up to 2 × 10 13 /cm 2 . A<br />

maximum shift in the threshold voltage <strong>of</strong> 3.2 V was<br />

achieved <strong>for</strong> the trilayer structure <strong>of</strong> LAO(8 nm)/Ge_NCs/<br />

LAO(3 nm)/Si. Ge NC FGs showed excellent charge<br />

retention time, whereas the decay in memory capacitance<br />

after 10 4 s <strong>of</strong> stress under a flat band voltage was only 8%.<br />

Kim et al. compared memory characteristics <strong>of</strong> SiGe NCs<br />

embedded in HfO2 or SiO2 dielectric layers. 558 Reported<br />

results indicated that the HfO2 tunneling oxide with SiGe<br />

NCs shows a faster charge carrier trapping and detrapping

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