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Improved electrical characteristics and reliability of MILC poly-Si TFTs using fluorine-ion implantation

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990 IEEE ELECTRON DEVICE LETTERS, VOL. 28, NO. 11, NOVEMBER 2007

Improved Electrical Characteristics and Reliability of

MILC Poly-Si TFTs Using Fluorine-Ion Implantation

Chih-Pang Chang and YewChung Sermon Wu

Abstract—In this letter, fluorine-ion (F+) implantation was employed to improve the electrical performance of metal-induced lateral-crystallization (MILC) polycrystalline-silicon thin-film transistors (poly-Si TFTs). It was found that fluorine ions mini-mize effectively the trap-state density, leading to superior electri-cal characteristics such as high field-effect mobility, low threshold voltage, low subthreshold slope, and highON/OFF-current ratio. F+-implanted MILC TFTs also possess high immunity against the hot-carrier stress and, thereby, exhibit better reliability than that of typical MILC TFTs. Moreover, the manufacturing processes are simple (without any additional thermal-annealing step), and compatible with typical MILC poly-Si TFT fabrication processes. Index Terms—Fluorine-ion implantation, metal-induced lateral crystallization (MILC), polycrystalline-silicon thin-film transis-tors (poly-Si TFTs).

I. INTRODUCTION

L

OW-TEMPERATURE polycrystalline-silicon thin-film transistors (poly-Si TFTs) have attracted considerable interest for their use in active-matrix liquid-crystal displays because they exhibit good electrical properties and can be integrated in peripheral circuits on inexpensive glass substrates [1]. As poly-Si TFTs require glass substrates, intensive studies have thus been carried out, reducing the crystallization tem-perature of amorphous silicon (α-Si) films. Ni-metal-induced lateral crystallization (MILC) is one of these efforts. In MILC, Ni islands are selectively deposited on top of α-Si films and allowed to crystallize at a temperature below 600C [2], [3].

Unfortunately, the poly-Si grain boundaries trap Ni and NiSi2precipitates, thus increasing leakage current and shifting

the threshold voltage [4]–[8]. A hydrogen plasma-treatment process has been utilized to reduce the trap states of poly-Si film to improve the device performance [9]. However, not only was it difficult to control hydrogen concentration in the poly-Si film but the formed Si–H bonds were also not strong enough to avoid the hot-carrier generation. Fluorine (F)-ion incorporation has been applied in the manufacturing of many electronic devices [10], [11]. On poly-Si TFTs implanted with fluorine, the Si–F bonds can eliminate the trap-state density, thus enhancing the performance of n-channel TFTs.

In this letter, a new manufacturing method for MILC poly-Si TFTs using fluorine-ion implantation was proposed. This

un-Manuscript received July 3, 2007. This work was supported by the Na-tional Science Council of China under Grants NSC95-2221-E009-087MY3 and NSC95-2221-E009-125. The review of this letter was arranged by Editor J. Sin. The authors are with the Department of Materials Science and Engineer-ing, National Chiao Tung University, Hsinchu 300, Taiwan, R.O.C. (e-mail: sermonwu@stanfordalumni.org).

Digital Object Identifier 10.1109/LED.2007.906803

complicated and effective method involves implanting fluorine atoms into poly-Si films, which produces MILC poly-Si TFTs of high performance and high reliability.

II. EXPERIMENT

A 100-nm-thick undoped (α-Si) layer was deposited onto a 500-nm-thick oxide-coated silicon wafer by low-pressure chemical-vapor-deposition (LPCVD) system. The photoresist was patterned to form desired Ni lines, and a 20-Å-thick Ni film was deposited on the α-Si, subsequently annealed at 540 C for 18 h to form the MILC poly-Si film. To reduce Ni contamination, the unreacted Ni metal was removed by chemical etching. The islands of poly-Si regions on the wafers were defined by reactive-ion etching; fluorine ions were then implanted into the MILC film. The projection range of fluorine ions was set at the middle of MILC layer. The dosage of fluorine ions and ion-accelerating energy was 2× 1013 cm−2 and 30 KeV, respectively. Next, a 100-nm-thick gate insulator was deposited by plasma-enhanced CVD. Then a 200-nm-thick poly-Si film was deposited for gate electrodes by LPCVD. After defining the gate, self-aligned 40 KeV P ions were implanted at a dose of 5× 1015cm−2to form the source/drain and gate. The F+-implanted MILC film and the P-implanted

source/drain/gate were then annealed/activated at 600 C for 24 h. Moreover, the manufacturing processes without any ad-ditional thermal annealing step and compatible with typical MILC poly-Si TFT fabrication processes.

III. RESULTS ANDDISCUSSIONS

Fig. 1 shows the ID–VGtransfer characteristics for the MILC poly-Si TFTs, with and without F+implantation. The measured and extracted key device parameters are summarized in Table I. The performance of F+-implanted TFTs was far superior to

that of MILC TFTs. This indicates the trap-state density (Nt) was effectively terminated using F+ implantation. The

trap-state density was extracted using Levinson’s and Proano’s method, which can estimate the Nt from the slope of the linear segment of ln[IDS/(VGS–VFB)] versus 1/(VGS–VFB)2

at low VDS and high VGS, where VFB is defined as the gate

voltage that yields the minimum drain–current at VDS= 0.1

[12], [13]. The trap density of F+-implanted MILC TFTs is 4.24× 1012 cm−2, which is less than that of MILC TFTs (6.29× 1012 cm−2). The reduction in Nt values implies that those defects have been terminated using F+ implantation. As a result, the carrier mobility increases. The minimum

OFF-current of the F+-implanted device, however, did not

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CHANG AND WU: IMPROVED ELECTRICAL CHARACTERISTICS AND RELIABILITY OF MILC POLY-Si TFTs 991

Fig. 1. Typical IDS–VGStransfer characteristics of the MILC poly-Si TFTs,

with and without F+implantation.

TABLE I

DEVICECHARACTERISTICS OF THEMILC POLY-Si TFTs, WITH ANDWITHOUTF+IMPLANTATION

change much. Similar performances and defects have been previously reported in other poly-Si TFTs that were passivated by the F+implantation [14]–[16].

In MILC poly-Si, there are two kinds of defects related to trap-state density: 1) Ni-related defects and 2) grain-boundary defects. Most of Ni-related defects were located at poly-Si/ buffer-oxide interface and grain boundaries, which trap Ni and NiSi2 precipitates [4]–[8]. Ni-related defects would

de-grade electric performance because the trap states introduced dangling and strain bonds. Secondary-ion mass spectroscopy (SIMS) was used to study the distribution of Ni and F. Fig. 2 shows the depth profile of the F+-implanted MILC poly-Si/ buffer-oxide structure after thermal annealing at 600 C for 24 h. High-Ni and high-F contents are both present at the MILC poly-Si/buffer-oxide interface. This observation suggested that F ions have diffused to the interface/boundaries to terminate Ni-related trap states and lead to improve electrical characteristics. On the other hand, the trap states in the grain boundaries will also increase the leakage current. Use of F atoms to fluorinate Si films can improve performance and reliability of poly-Si TFTs [16]. This is because F atoms can terminate dangling bonds and replace weak bonds in the grain boundaries and

Fig. 2. SIMS depth profile of nickel and fluorine in the structure of MILC poly-Si channel/buffer-oxide.

Fig. 3. Threshold-voltage variation versus stress time for the MILC poly-Si TFTs, with and without F+implantation.

SiO2/poly-Si interface and, thus, reduce the trap states in the

poly-Si channel. As a result, the carrier mobility increases due to the decrease in the boundary scattering by passivation-of-boundaries defects. However, the minimum OFF-currents were nearly unchanged [14]–[16].

The other important issue of poly-Si TFTs is their reliability, which was examined under hot-carrier stress. As shown in Figs. 3 and 4, the threshold voltage and the ON-current of TFTs were degraded, because dangling bonds are created due to the trapping of electrons at weak Si–Si and Si–H bonds [17], [18]. Compared with those of typical MILC TFTs, the threshold voltage andON-current degradations of F+-implanted

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992 IEEE ELECTRON DEVICE LETTERS, VOL. 28, NO. 11, NOVEMBER 2007

Fig. 4. ON-current degradation versus stress time for the MILC poly-Si TFTs, with and without F+implantation.

MILC TFTs are greatly improved by the implantation process. F+-implanted MILC TFTs also possess high immunity against the hot-carrier stress and, thereby, exhibit lower ∆VTH and

∆ION/ION than that of typical MILC TFTs. In other words,

weaker Si–H and Si–Si bonds were replaced by stronger Si–F bonds, which could not be broken under hot-carrier stress, thus leading to improved electrical reliability.

Electrical properties of the F+-implanted MILC TFTs with heavy implantation dosages (2× 1014 and 2× 1015 cm−2) were also studied in this letter. It is found that the electrical characteristics of MILC TFT are degraded as the implantation dosage increases. When the dosage reached 2× 1015 cm−2, the device performance was very poor. This is because, when the implantation dosages are higher than Si solid solu-bility, the trap-state density and fluorine clusters increased with the dosage [19].

IV. CONCLUSION

An investigation of the effects of F+-implantation process

on the electrical characteristics and reliability of MILC poly-Si TFTs has led to the development of a simple effective process for improving the TFT electrical properties. Results show that, compared with typical MILC TFTs, F+-implanted

TFTs exhibit higher field-effect mobility, superior subthreshold slope, lower threshold voltage, higher ON/OFF-current ratio, and lower trap-state density (Nt). It was also found that F+ -implantation process can greatly alleviate the threshold voltage and the ON-current degradations under hot-carrier stress. F+ -implanted MILC TFTs possess high immunity against the hot-carrier stress and, thereby, exhibit lower ∆VTHand ∆ION/ION

than that of typical MILC TFTs. This is because the weaker Si–H and Si–Si bonds were replaced by stronger Si–F bonds, which could not be broken under hot-carrier stress, thus leading to improved electrical reliability.

ACKNOWLEDGMENT

The authors would like to thank the technical support from the National Nano Device Laboratory of NSC and Nano Facil-ity Center of National Chiao Tung UniversFacil-ity.

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數據

Fig. 1. Typical I DS –V GS transfer characteristics of the MILC poly-Si TFTs,
Fig. 4. ON -current degradation versus stress time for the MILC poly-Si TFTs, with and without F + implantation.

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