Supporting Information Sakurai-etal Revised · Shunsuke Sakurai, Maho Yamada, Hiroko Nakamura,...

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1 Supplementary Information A Phenomenological Model for Selective Growth of Semiconducting Single-Walled Carbon Nanotube Based on Catalyst Deactivation Shunsuke Sakurai, Maho Yamada, Hiroko Nakamura, Atsuko Sekiguchi, Fumiaki Tanaka, Don N. Futaba, and Kenji Hata* National Institute of Advanced Industrial Science and Technology (AIST), Central 5, 1-1-1, Higashi, Tsukuba, Ibaraki, 305-8565, Japan. * Author to whom correspondence should be addressed. 1. Measurement and minimization of the background gas level in the furnace In this study, the background oxidative gases has been minimized mainly by the following three measures. First, the gas exchange chamber (Fig. 3a) was equipped to prevent the contamination of oxygen and water vapor from outside of the furnace. Second, to avoid the generation of carbon monoxide (CO) via the reaction between carbon dirt impurities in the furnace and water vapor during the catalyst conditioning process (water gas reaction: C + H2O → CO + H2), furnace tube and sample holders made of quartz were heated (800 °C, 10 minutes) in an O2 atmosphere (diluted to about 20% with He) before each CVD process. Using Fourier transform infrared spectroscopy (Thermo scientific, Nicolet6700), we confirmed that CO concentration in the emitted gas from the furnace during CVD processes is less than 0.1 ppm, it reached up to 20 ppm without O2 cleaning. Third, after O2 cleaning, the furnace and sample holders were annealed in a hydrogen atmosphere (100%) for 5 minutes to decrease oxygen atoms adsorbed on the furnace. During this hydrogen annealing, water concentration in the exhausted gas typically reached to 100 ppm. By inserting this hydrogen annealing process, the increase in water vapor concentration during the catalyst formation process was less than 2 ppm. 2. Supplemental Raman spectra Electronic Supplementary Material (ESI) for Nanoscale. This journal is © The Royal Society of Chemistry 2015

Transcript of Supporting Information Sakurai-etal Revised · Shunsuke Sakurai, Maho Yamada, Hiroko Nakamura,...

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    Supplementary Information

    A Phenomenological Model for Selective Growth of

    Semiconducting Single-Walled Carbon Nanotube Based on

    Catalyst Deactivation

    Shunsuke Sakurai, Maho Yamada, Hiroko Nakamura, Atsuko Sekiguchi, Fumiaki Tanaka,

    Don N. Futaba, and Kenji Hata*

    National Institute of Advanced Industrial Science and Technology (AIST), Central 5, 1-1-1,

    Higashi, Tsukuba, Ibaraki, 305-8565, Japan.

    *Author to whom correspondence should be addressed.

    1. Measurement and minimization of the background gas level in the furnace

    In this study, the background oxidative gases has been minimized mainly by the

    following three measures. First, the gas exchange chamber (Fig. 3a) was equipped to prevent the

    contamination of oxygen and water vapor from outside of the furnace. Second, to avoid the

    generation of carbon monoxide (CO) via the reaction between carbon dirt impurities in the

    furnace and water vapor during the catalyst conditioning process (water gas reaction: C + H2O

    → CO + H2), furnace tube and sample holders made of quartz were heated (800 °C, 10 minutes)

    in an O2 atmosphere (diluted to about 20% with He) before each CVD process. Using Fourier

    transform infrared spectroscopy (Thermo scientific, Nicolet6700), we confirmed that CO

    concentration in the emitted gas from the furnace during CVD processes is less than 0.1 ppm, it

    reached up to 20 ppm without O2 cleaning. Third, after O2 cleaning, the furnace and sample

    holders were annealed in a hydrogen atmosphere (100%) for 5 minutes to decrease oxygen atoms

    adsorbed on the furnace. During this hydrogen annealing, water concentration in the exhausted

    gas typically reached to 100 ppm. By inserting this hydrogen annealing process, the increase in

    water vapor concentration during the catalyst formation process was less than 2 ppm.

    2. Supplemental Raman spectra

    Electronic Supplementary Material (ESI) for Nanoscale.This journal is © The Royal Society of Chemistry 2015

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    Raman shift (cm−1)

    Inte

    nsity

    (a.u

    .)

    532 nm

    Selective CVD

    1700 1600 1500 1400 1300 1200

    Raman shift (cm−1)

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    nsity

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    532 nm

    Non-selective CVD

    1700 1600 1500 1400 1300 1200

    Raman shift (cm−1)

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    nsity

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    532 nm

    300 250 200 150 100Raman shift (cm−1)

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    300 250 200 150 100

    Raman shift (cm−1)

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    nsity

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    633 nm

    300 250 200 150 100Raman shift (cm−1)

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    nsity

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    Raman shift (cm−1)

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    .)

    785 nm

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    Raman shift (cm−1)

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    a.u

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    (a)

    (b)

    (c)

    (d)

    AverageAverage

    Average

    Average

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    AverageAverage

    Figure S1. Raman spectra of selective (left) and non-selective CVD (right) collected from

    more than 25 positions. Red spectra show the average of spectra from all positions. (a)

    Spectra showing G-band region (excitation wave length: 532 nm). (b) Spectra showing

    RBM peaks (excitation wave length: 532 nm). (c) Spectra showing RBM peaks (excitation

    wave length: 633 nm). (d) Spectra showing RBM peaks (excitation wave length: 785 nm).

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    H2O 0.25 % 0.5 % 1 % 1.5 % 2 %

    0 ppm

    2 ppm

    10 ppm

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    50 ppm

    Raman shift (cm-1)

    H2

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    H2O 0.25 % 0.5 % 1 % 1.5 % 2 %

    0

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    Figure S2. Raman spectra showing RBM peaks of SWCNTs synthesized with different

    water and hydrogen amounts during catalyst conditioning process. Upper: excitation

    wavelength of 532 nm, lower: 785 nm.

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    300 200 100300 200 100

    Raman shift (cm-1) Raman shift (cm-1)

    785 nm532 nm

    S22

    M11

    3. Reference experiment feeding water vapor during SWCNT growth process

    To exclude the possibility that the selective etching of m-SWCNT, previously reported

    mechanism of selective growth, worked mainly in the current work, a reference SWCNT growth

    experiment was conducted by the following process. Catalyst formation process was conducted

    as same as described in the manuscript. Then, without catalyst conditioning process, water vapor

    (50 ppm) and hydrogen (0.25%) was introduced into the furnace during SWCNT growth process

    with ethylene flow (0.25%). Raman spectra (Figure S4) shows a significant RBM peaks

    corresponding to m-SWCNT, resulting in a greatly decreased selectivity of Psmall = 53% from

    CVD process with catalyst conditioning process using same amount of water and hydrogen.

    M11

    S33

    M11

    S22

    785 nm

    532 nm

    Si

    Raman shift (cm−1)

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    (a.

    u.)

    100200300

    Figure S4. Raman spectra of SWCNTs synthesized in the reference experiment. Upper: 532

    nm excitation wavelength, lower: 785 nm. Raman shift regions indicated by red and blue

    squares represent the signals from m-SWCNT and sc-SWCNT, respectively.

    Figure S3. Raman spectra of HiPco. Left: 532 nm excitation wavelength, right: 785 nm.