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Switch-on Phenomena and Field Emission from Single-Walled Carbon Nanotubes Embedded in Glass
Applied Microscopy 2017;47:86-94
Published online September 30, 2017
© 2017 Korean Society of Microscopy.

Samer I. Daradkeh, and Marwan S. Mousa*

Department of Physics, Mu’tah University, Al-Karak 61710, Jordan
Correspondence to: Mousa MS, Tel: +962-79-565-9761, Fax: +962-3-2375540, E-mail:
Received August 18, 2017; Revised September 7, 2017; Accepted September 8, 2017.
This is an open-access article distributed under the terms of the Creative Commons Attribution Non-Commercial License ( which permits unrestricted noncommercial use, distribution, and reproduction in any medium, provided the original work is properly cited.

In this study, we will describe a new design of carbon nanotubes tip. Single-walled carbon nanotubes produced using high-pressure CO over Fe particles (HiPCO) at CNI, Houston, TX used in this study. These tips were manufactured by employing a drawing technique using glass puller. Field electron microscopies with tips (cathode) to screen (Anode) separation of ~10 mm was used to characterize the electron emitters. The system was evacuated down to base pressure of (~10−8 mbar) when baked at up to (~200°C) over night. An electron field emission patterns, as well as current versus voltage characteristics and Fowler-Nordheim plots, are discussed.

Keywords : Cold field emission, Single-walled carbon nanotubes, Fowler-Nordheim plot

Electron source plays an essential role in the information display. They mostly use the thermionic emission mechanism, where the electrons are emitted from heated filaments (hot cathode) (Modinos, 1984). Field emission is an alternative mechanism to extract electron where electron emitted from a surface by tunneling from a state near the Fermi level. There are several materials used for field electron emission but the most promising one is carbon nanotubes (CNTs) (Forbes, 2012; Forbes et al., 2015).

CNTs are composed of graphite sheets rolled into seamless hollow cylinders with diameter ranging from (1 nm) to about (50 nm) (Saito & Uemura, 2000), CNTs discovered by lijima (1991) and it have been attached much attention as electron source for many reasons such as ultra-small radius, high aspect ratio, high electrical conductivity (Zhang et al., 2005), high chemical stability and high mechanical strength (Bani Ali & Mousa, 2016), CNTs offer several advantages over other emitters material such as enhanced current stability, low threshold voltage, long lifetime (Hong et al., 2009) and high emission current density. These emission characterizations are directly related to the unique structure and chemical bonding of the CNTs (Cheng & Zhou, 2003). And for previous reason, we use single-walled carbon nanotubes (SWCNTs) to study the field electron emission.



Field electron emission was explained in 1928 by combining quantum tunneling theory with Fermi-Dirac statistical theory. The theory of field electron emission from bulk metals was proposed by Ralph H. Fowler and Lothar W. Nordheim, this phenomenon can be described by a family of the approximate equation called “Fowler-Nordheim type equation”, is named after them. Strictly speaking, these equations apply only to field emission from bulk metal, but the theory often used—as a rough approximation—to describe field emission from other material (Ala’a et al., 2015). The original Fowler-Nordheim type (FN-type) equation was developed using several hypotheses and some simplify assumption. Thus FN: (1) assumed a smooth, flat, planar emitter surface, with constant electric field outside it; (2) disregarded details of emitter atomic structure; (3) ignored what would now be called the exchange-and-correlation interaction between the escaping electron and the emitter surface; (4) assumed a Sommerfeld-type free-electron model for the emitter electron states; (5) assumed electrons obeyed Fermi-Dirac statistics; and (6) approximated emitter temperature as 0 K (Forbes, 2012).

Cold field emission (CFE) from bulk metals is described by a family of the approximate equation called FN-type equations. These equations were derived for material situations where emission comes from a degenerate metal like conduction band of sufficient depth, and quantum-confinement effects (Forbes, 2010; Qin et al., 2011).

The equations have involved repeated improvement and reformulation of theoretical approaches, the Table 1 show how FN equation developed over years (Forbes, 2010).

And the development still going on to apply the FN equation on the nanoscopic field emitter, more specifically in (Edgcombe, 2005) and (Edgcombe & Jonge, 2007) develop a formula used for sphere on a cone model (large anode-tip distance), other works are, the hyperboloid by (Zuber et al., 2002) in which the emission from a single surface element dS in considered to be FN type, and the derive a generalized FN equation for nanoscopic field emitters by (Kyritsakis & Xanthakis, 2014).

Experimental Setup

This study uses SWCNTs are produced by catalytic conversion of high-pressure CO over Fe particle (HiPCO) processed at CNI, Houston, TX, where the length of individual and SWCNT is approximately 1~3 μm, and the mean diameter is 1~4 nm, and the emitter produced by using a “glass puller” to, it’s a technique for pulling heated glass capillary tubes into fine points. The apparatus is shown in Fig. 1.

Two bearing are located accurately on plates supported by three stainless steel rods fixed rigidly to the frame of the unit control unit. This frame is strong enough to serve as a stable base for the instrument. The glass tube fits inside these bearings between the upper and lower chucks with the furnace loop located around it. The lower chuck spindle slides vertically to pull down the glass tube under the influence of gravity. As the temperature of the furnace is raised to the soften point of the glass the tube necks as shown in Fig. 1 (Mousa & Hibbert, 1993), the SWCNTs were entered into the opposite end of each glass tube so they would protrude at the tip end, the final result as shown in Fig. 2 (Marwan et al., 2015).

The sample placed inside ultra-high vacuum system which the axial tip-to-screen separation was fixed at around (10 mm). The standard producer was to bake out the system at ~200°C for 12 hours, obtaining the vacuum down to ~10−8 mbar (Madanat et al., 2015; Mousa, 2007).

The commonest method of investigating emitter behavior is to measure current-voltage (I–V) characteristics and extract one or more characterization parameters from FN plot (i.e., a plot of the form In(I/V2) vs. 1/V, or using equivalent using other variables (Forbes et al., 2015).


In operation, the field emission microscope (FEM) applied voltage (V) is increased slowly until a “switch on voltage” (VSW) is reached where the emission current suddenly changes from an effective zero to saturation value (ISAT), then by slowly decreasing the switching voltage to lower value the emission current starts to be decreasing until limit reached, beyond which the emission current falls smoothly to zero as the applied voltage is decreased the threshold value (VTH). However, as shown in Fig. 3, this part of the characteristics can be routinely divided into three region, (region 1) were bounded by the voltage (VL) and the threshold voltage (VTH), (region 2) bounded by the voltage (VL) and (VSAT) and (region 3) confined between (VSAT) to (VMAX) that is the maximum voltage before the tip explodes (Ala’a et al., 2015; Mousa, 1991).

To obtain quantitative information about the microscopic properties of the emitter regime, the total electron emission current (I) has been plotted as a function of the applied voltage V between the emitter and the anode. Emission characterization will be presented as I–V plots and as the related FN plots. Throughout the experiments, electron emission image has been recorded by means of a digital camera, in order to study the spatial distribution and stability of the emission current. The test was performed under a vacuum pressure of 9×10−8 mbar.

As the voltage increased slowly, in Fig. 4A and C, the characteristics of the emitter is shown the electron emission initiated at an applied voltage=750 V with current 2 pA, and by increasing the applied voltage slowly caused an increasing in emission current, and suddenly the emission current raise to 3 μA at voltage value 2,550 V, Fig. 4B shows the emission image at VSW=2,550 V, ISW=3 μA.

In Fig. 5A, by decreasing voltage slowly, the characteristics of the emitter show that the saturated region extends down to the value VSAT=1,050 V, with ISAT=3.99 μA, and then started to fall smoothly to VTH=750 V with I=5 pA, as shown in Fig. 5B, once the emitter leaves saturation, the (decreasing) current-voltage relationship generate an approximately linear FN plot, with slope about −16028.2 decade V.

The experiment was repeated under the same condition. The Fig. 6A shows the relation between current-voltage for the same tip (CNT-10) for both increasing and decreasing voltage, and the current emission image at VSW and VSAT value. By increasing the applied voltage until point VSW=1,400 V was reached the current emission suddenly increased to ISW=5.10 μA, and by decreasing the voltage, the emission current saturated to VSAT=1,150 V with ISAT=1.30 μA, by further decreasing the voltage, the emission current continue decreasing until VTH=950 V was reached with current emission value 30 pA, then it vanishes.

Studies also carried out on a second tip (CNT-11) where Fig. 7 shows the optical micrograph to it at 50× magnifications, which is shows the protrude CNT from it under a vacuum pressure of 3×10−8 mbar, the voltage was applied and the I–V characteristics were recorded. Emission started at 500 V with current 10 pA, by increasing the applied voltage slowly the current emission suddenly increased at applied voltage value VSW=1,700 V with current emission ISW=8.7 μA. Fig. 8 shows the related plots. By decreasing the applied voltage the I–V characteristics and FN plot as shown in Fig. 9 that the emitter (CNT-11) shows saturation in current emission at applied voltage VSAT=850 V, with ISAT=1.18 μA. Fig. 10C shows the emission image at multiple applied voltages.

The experiment was repeated after allowing relaxation which we leave the sample under vacuum for 5 hours with no applied voltage at same vacuum pressure value. The current-voltage characteristics Fig. 11 shows initiation by low current emission at 500 V, with an emission current of 1 Pa, as shows the switch-on at VSW=1,600 V, ISW=3.1 μA, we increased the applied voltage to V=1,800 V, it gave emission current 8.92 μA. As the voltage reduced, the “saturated” region extends down to value VSAT=800 V, ISAT=1.8 μA as it appeared in Fig. 12. Further voltage reduction causes the emission current to fall to nearly zero, reaching the threshold voltage VTH=450 V, ITH=6 pA.


It is helpful to attempt to understand the conditions under which continuous stable current may flow from the composite emitters. The electron emission dynamics is mostly controlled by the metal/glass interface. Our experiment shows that we can obtain high emission current from SWCNTs. Some of the emitters experienced some fluctuation and some of them show a stable emission current at high emission current.


There is fluctuation in the emission current due to the nonmetallic nature of the tip, field penetration and fluctuations of the applied potential shift the position of the emitting level, the other possibility is because of the structure of the cap, whereas it is well-known that small changes in adsorbate coverage result in large variations of the work function (Minoux et al., 2005), that could lead to observed saturation at high applied voltages and strong instabilities of the emission in some voltages ranges (Binh et al., 1996; Swanson & Bell, 1973), once the adsorbates removed, the emission current will be reduced because these adsorbates enhanced the field emission current of nanotube by two or three order (Dean & Chalamala, 2000) and the deviation from FN equations will disappear.

The effect of relaxation process on field emission process from SWCNT could reduce the VSW as we observed in CNT-11.


The authors would like to thank Deanship of the Academic Research at Mu’tah University for supporting this work. Authors acknowledge Prof. Dr. M-Ali H. Al-Akhras for providing the SWCNTs and CNTFs.

Fig. 1. Schematic diagram of the glass puller. SWCNTs, single-walled carbon nanotubes.
Fig. 2. Optical micrograph of (CNT-10) tip at 50× magnification. CNT, carbon nanotubes.
Fig. 3. The generalized form of the current-voltage (I–V) characteristics.
Fig. 4. Increasing voltage CNT-10. (A) Current-voltage (I–V) characteristics shows VSW=2,550 V, ISW=3 μA. (B) Emission image at VSW. (C) Fowler-Nordheim (FN) plot with slope −9256.25. (D) Increasing voltage CNT-10 tip, Emission image V=2,100 V, I=2.0 μA. CNT, carbon nanotubes.
Fig. 5. Decay V CNT-10. (A) Current-voltage (I–V) characteristics shows switch-on at VSW=2,810 V, ISW=18.1 μA. (B) Fowler-Nordheim (FN) plot. (C) Emission image at VSW. CNT, carbon nanotubes.
Fig. 6. Increasing and decreasing V CNT-10. (A) Current-voltage (I–V) characteristics. (B) Fowler-Nordheim (FN) plot with slope −32580.8 decayed V. (C) Emission image at 1,340 V. (D) Emission image at VSW. CNT, carbon nanotubes.
Fig. 7. CNT-11 optical micrograph at 50× magnification. CNT, carbon nanotubes.
Fig. 8. Emitter (CNT-11), increasing voltage. (A) Current-voltage (I–V) characteristics. (B) Related Fowler-Nordheim (FN) plot. The applied voltage is in range of 500 to 2,550 V. CNT, carbon nanotubes.
Fig. 9. Emitter (CNT-11), decay V. (A) Current-voltage (I–V) characteristics. (B) Related Fowler-Nordheim (FN) plot with slope about −2533.33. CNT, carbon nanotubes.
Fig. 10. Decreasing voltage, emission images. (A) V=2,450 V, I=13.1 μA. (B) V=2,480 V, I=13.3 μA. (C) V=2,500 V, I=13.7 μA.
Fig. 11. Increasing voltage, tip CNT-11. (A) Current-voltage (I–V) characteristics. (B) Fowler-Nordheim (FN) plot. (C) Emission image at V=1,800 V, I=8.92 μA. CNT, carbon nanotubes.
Fig. 12. Decay V, (CNT-11). (A) Current-voltage (I–V) characteristics. (B) Fowler-Nordheim (FN) plot. (C) Field electron microscope image at V=1,730 V, I=8.1 μA. CNT, carbon nanotubes.

The development of FN equations

FN-type equationArea of useIdentify terms
JL=aϕ-1FL2exp(-bϕ32/FL)Elementary, for LECDϕ: work function
a&b: first and second FN constant
FL: local surface electric field
JL=PFNaϕ-1FL2exp(-bϕ32/FL)Original, for LECDPFN: tunneling prefactor
JL=tF-2aϕ-1FL2exp(-vFbϕ32/FL)Standard or Murphy-Good equation, for LECDtF & vF: particular value of mathematical function v and t, where v and t are sometimes called field emission elliptic function.
JL=λLaϕ-1FL2exp(-vFbϕ32/FL)Technically complete, for LECD emitterλL: pre-exponential correction factor
JM=αMλCaϕ-1γC2FM2exp(-vFbϕ32/FL)Technically complete, for LAFEγC: characteristics macroscopic field enhancement factor and defined by (FC/FM)

FN, Fowler-Nordheim; LECD, local emission current density; LAFE, large area field emitter.

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