2015
DOI: 10.1016/j.physe.2015.06.030
|View full text |Cite
|
Sign up to set email alerts
|

Observation of room temperature negative differential resistance in solution synthesized ZnO nanorod

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

1
5
0

Year Published

2016
2016
2021
2021

Publication Types

Select...
4
1

Relationship

0
5

Authors

Journals

citations
Cited by 5 publications
(6 citation statements)
references
References 11 publications
(11 reference statements)
1
5
0
Order By: Relevance
“…The negative differential resistance properties are observed on various materials with different morphology such as ZnO nanorod, porous silicon devices and graphene nanoribbon FET [38,64,65]. The NDR property of NiFe 2 O 4 nanowire device is similar to the reported works, which further strengthens the present work.…”
Section: I-v Characteristics Of Nife 2 O 4 Nanowire Devicesupporting
confidence: 89%
“…The negative differential resistance properties are observed on various materials with different morphology such as ZnO nanorod, porous silicon devices and graphene nanoribbon FET [38,64,65]. The NDR property of NiFe 2 O 4 nanowire device is similar to the reported works, which further strengthens the present work.…”
Section: I-v Characteristics Of Nife 2 O 4 Nanowire Devicesupporting
confidence: 89%
“…During bias sweep from 0 V → −2 V (sweep 3), the current in the LRS raises until −0.8 V (for 200 nm CS, figure 2(f)) but decreases with a further increase in bias. This is a characteristic of NDR behavior, often observed in organic memory devices [38][39][40][41]. While increasing bias from −2 V → 2 V (sweep 4, 5), the device makes a transition to HRS.…”
Section: Resultsmentioning
confidence: 81%
“…To explore NDR in our devices, we also performed I-V measurements for the device with a 200 nm thick CS layer with the variations in voltage step (or scan rate) and bias stress, which is displayed in figures 3(a) and (b). The property of decreasing current with increasing applied bias (at different scan rates) is attributed to the NDR nature, which is highly desired for high-frequency applications [41,50]. The peak current (NDR peak) of the devices near −0.45 V (figure 3(a)) improved from 8 nA to 55 nA with the voltage step variation (0.005 V to 0.25 V).…”
Section: Resultsmentioning
confidence: 99%
“…Noticeably, the NDR phenomenon became slightly weak and the PVCR decreased at a higher temperature of 80 • C or even disappeared completely at 120 • C. Typically, the effect of NDR is observed at lower temperatures, and the carriers can tunnel from the diamond valence band to the ZnO defect band at 20 and 80 • C (Figures 4A,B). While at 120 • C, PVCR is reduced and, thus, leads to the disappearance of NDR due to enhanced thermionic emission current and variation of energy band (Kathalingam et al, 2015). As shown in the schematic energy band diagram (Figure 4C), the Fermi level moved up and entered into the bandgap at 120 • C. The n-ZnO NRs and p-degenerated diamond semiconductor were approaching the intrinsic semiconductor.…”
Section: Resultsmentioning
confidence: 97%
“…Typically, the effect of NDR is observed at lower temperatures, and the carriers can tunnel from the diamond valence band to the ZnO defect band at 20 and 80°C ( Figures 4A,B ). While at 120°C, PVCR is reduced and, thus, leads to the disappearance of NDR due to enhanced thermionic emission current and variation of energy band (Kathalingam et al, 2015 ). As shown in the schematic energy band diagram ( Figure 4C ), the Fermi level moved up and entered into the bandgap at 120°C.…”
Section: Resultsmentioning
confidence: 99%