Elsevier

Thin Solid Films

Volume 572, 1 December 2014, Pages 15-19
Thin Solid Films

Structural evolution of bias sputtered LiNi0.5Mn1.5O4 thin film cathodes for lithium ion batteries

https://doi.org/10.1016/j.tsf.2014.08.034Get rights and content

Highlights

  • LiNi0.5Mn1.5O4 thin films have been deposited on stainless steel substrates.

  • Various negative biases were applied on the substrates during deposition.

  • The particle sizes of LNMO thin films decrease with increasing negative bias.

Abstract

LiNi0.5Mn1.5O4 (LNMO) thin films have been deposited on stainless steel substrates using radio frequency (f = 13.56 MHz) magnetron sputtering, followed by thermal annealing in ambient atmosphere. Various negative biases were applied on the substrates during deposition. The structural evolution of LNMO thin films under different negative biases has been investigated and characterized by X-ray diffraction. All of the deposited films exhibit a crystalline spinel structure with a space group of Fd-3m, which is a so-called disordered phase. The results also indicate that particle size decreases with increasing negative bias. The electrochemical properties of the LNMO thin films as cathode materials for lithium ion batteries were investigated. Two distinctive voltage plateaus at ~ 4.7 V and at ~ 4.0 V (vs. Li+/Li) can be observed in the discharge curves, corresponding to the reactions of the disordered phase. The capacity of LNMO thin film electrodes under suitable negative bias can be optimized.

Introduction

Lithium ion batteries have been widely used as energy sources for portable electronic devices in the past few decades. Recently, hybrid electric vehicles, power tools, and other multi-functional devices have demanded lithium ion batteries with a high power density [1]. In this regard, high operating voltage cathode materials have been extensively studied.

The spinel LiMn2O4 has great promise for future use in lithium ion batteries because of its low cost, high abundance, environment friendliness, and safety [2]. LiMn2O4 also possesses a relatively high voltage of ~ 4.0 V, or over 4.5 V (vs. Li+/Li), after transition metal substitution, which makes it more suitable for high power applications than other cathode materials [3]. However, LiMn2O4 has limitations such as Mn3 + dissolution at high temperatures (> 55 °C) and Jahn–Teller distortion at low voltage (2.8 V), causing structure instability and leading to poor cycling stability [2], [4]. Therefore, cathode materials with high voltage and high stability are desirable. In this regard, 3d-transition metal (M) substitution of LiMn2O4 has been previously studied in the field [5]. The LiMxMn1  xO4 cathode materials can provide a high operating voltage of ~ 5 V vs. Li+/Li through the redox reaction of M3 + to M4 + for M is Cr or Co, and M2 + to M4 + for M = Ni [6]. In addition, Ni substitution can restrict the Mn ion dissolution by maintaining the Mn at valence state of 4 + [7]. Spinel LiNi0.5Mn1.5O4 (LNMO)1 is a promising candidate because the Ni substitution not only reduces the Mn3 + dissolution [8], [9], it also elevates the operating voltage (4.7 V vs. Li+/Li) [10], [11]. The high operating voltage may lead to the decomposition of electrolyte and that is known to induce the formation of a passive layer on the surface of the LNMO, causing the decay of the cycle life [12]. Therefore, various protective coatings on the surface of the LNMO have been studied [13].

Spinel LiMn2O4 is cubic with a space group of Fd-3m, where the Li atoms occupy the 8a site, Mn atoms the 16d site, and O atoms the 32e sites [14]. After Ni substitution, the structure of the LNMO is no longer that of a typical spinel. In the ordered phase of the LNMO, the Li atoms occupy 8c sites, Ni atoms and Mn atoms locate at the 4a and 12d sites, and O atoms inhabit the 8c and 24e sites (space group of P4332) [15]. When oxygen deficiency exists in the LNMO structure, impurity phases, such as LixNi1  xO and NiO, may occur [3], [16]. These impurity phases lead to the reduction of Mn4 + to Mn3 +. In order to maintain the valence state in the LNMO compound, some of the grains may crystallize into a so-called disordered phase [17], [18], where Li atoms locate at the 8a sites, Mn and Ni atoms are randomly distributed at the 16d sites, and O atoms occupy the 32e sites (space group of Fd-3m) [15].

Li–Ni–Mn–O related thin films have been fabricated by sputter deposition to study the influences of different Li+ stoichiometries [12]. The pure LNMO thin films without conducting additives and binders were found to be useful for scientific investigation. In the present study, the LNMO thin films were prepared by radio frequency (RF)2 magnetron sputtering deposition and then characterized [12], [13]. Analysis of the structural evolution and electrochemical properties of the LNMO films deposited under different substrate biases were performed. This study demonstrates that the bias applied onto the substrate can effectively modify the structure of the film resulting in different electrochemical characteristic toward lithium. The cycling tests of LiNi0.5Mn1.5O4 cells were directly affected by the electrolyte decomposition at high voltage (> 4.5 V) [13]. Therefore, this study is only focused on the relationship between the sputtering conditions, structural evolution, and related capacity within three cycles.

Section snippets

Experimental details

LNMO thin films were deposited on 316L type stainless steel (SS) substrates by radio frequency (RF) magnetron sputter deposition. The sputtering was carried out under constant pressure of 0.67 Pa (base vacuum 3.3 × 10 4 Pa) with Ar flow rate of 15 sccm. A pure LiNi0.5Mn1.5O4 target (Gredmann Ltd. 99.5%) of 5.08 cm diameter was used. RF power of 80 W was applied, and the target/substrate distance was fixed at 7.5 cm. The SS substrates were placed on a SS substrate holder that was grounded or negatively

Results and discussion

Fig. 1 displays the SEM micrographs of the prepared LNMO thin films. Although all of the LNMO films undergo the same post-annealing process, their surface morphologies varied with the different biases. As the bias exceeds − 10 V, the particle sizes decrease with the negative bias. For samples 0bias, 10bias, 30bias, and 50bias, the particle sizes are 600 nm, 600 nm, 100 nm, and 50 nm, respectively. For the sample deposited on the grounded substrate (sample 0bias), the LNMO thin film exhibits a rough

Conclusions

LNMO thin film electrodes have been fabricated using magnetron sputter deposition with various biases applied to the substrates. The structural evolution of LNMO is found to be considerably influenced by the bias. The grain size decreases with increasing substrate bias because of the high energy ion bombardment on the surface of the growing LNMO thin films. Consequently, the LNMO thin films demonstrate a high discharge capacity at a substrate bias of − 30 V. However, relatively low capacity is

Acknowledgments

The research work was sponsored by the National Science Council Taiwan under contract no. NSC 101-2632-E-035-002-MY3, NSC 102-2221-E-035-015, NSC 102-2218-E-035-011 and NSC 103-2218-E-035-004.

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