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دانلود کتاب Molecular Constants Mostly from Infrared Spectroscopy: Non-linear Triatomic Molecules, Part 1: H2O (HOH), Part ε: HD16O (H16OD), HT16O (H16OT), HD17O (H17OD), HD18O (H18OD), DT16O (D16OT)

دانلود کتاب ثابت‌های مولکولی عمدتاً از طیف‌سنجی فروسرخ: مولکول‌های سه اتمی غیر خطی، بخش 1: H2O (HOH)، بخش ε: HD16O (H16OD)، HT16O (H16OT)، HD17O (H17OD)، HD18O (H18OD)، DT16O (D1)

Molecular Constants Mostly from Infrared Spectroscopy: Non-linear Triatomic Molecules, Part 1: H2O (HOH), Part ε: HD16O (H16OD), HT16O (H16OT), HD17O (H17OD), HD18O (H18OD), DT16O (D16OT)

مشخصات کتاب

Molecular Constants Mostly from Infrared Spectroscopy: Non-linear Triatomic Molecules, Part 1: H2O (HOH), Part ε: HD16O (H16OD), HT16O (H16OT), HD17O (H17OD), HD18O (H18OD), DT16O (D16OT)

ویرایش: 1 
نویسندگان:   
سری: Molecules and Radicals 20C1ε 
ISBN (شابک) : 9783662493267, 9783662493274 
ناشر: Springer-Verlag 
سال نشر: 2016 
تعداد صفحات: 485 
زبان: English 
فرمت فایل : PDF (درصورت درخواست کاربر به PDF، EPUB یا AZW3 تبدیل می شود) 
حجم فایل: 7 مگابایت

قیمت کتاب (تومان) : 37,000



کلمات کلیدی مربوط به کتاب ثابت‌های مولکولی عمدتاً از طیف‌سنجی فروسرخ: مولکول‌های سه اتمی غیر خطی، بخش 1: H2O (HOH)، بخش ε: HD16O (H16OD)، HT16O (H16OT)، HD17O (H17OD)، HD18O (H18OD)، DT16O (D1): طیف سنجی و میکروسکوپی



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در صورت تبدیل فایل کتاب Molecular Constants Mostly from Infrared Spectroscopy: Non-linear Triatomic Molecules, Part 1: H2O (HOH), Part ε: HD16O (H16OD), HT16O (H16OT), HD17O (H17OD), HD18O (H18OD), DT16O (D16OT) به فرمت های PDF، EPUB، AZW3، MOBI و یا DJVU می توانید به پشتیبان اطلاع دهید تا فایل مورد نظر را تبدیل نمایند.

توجه داشته باشید کتاب ثابت‌های مولکولی عمدتاً از طیف‌سنجی فروسرخ: مولکول‌های سه اتمی غیر خطی، بخش 1: H2O (HOH)، بخش ε: HD16O (H16OD)، HT16O (H16OT)، HD17O (H17OD)، HD18O (H18OD)، DT16O (D1) نسخه زبان اصلی می باشد و کتاب ترجمه شده به فارسی نمی باشد. وبسایت اینترنشنال لایبرری ارائه دهنده کتاب های زبان اصلی می باشد و هیچ گونه کتاب ترجمه شده یا نوشته شده به فارسی را ارائه نمی دهد.


توضیحاتی در مورد کتاب ثابت‌های مولکولی عمدتاً از طیف‌سنجی فروسرخ: مولکول‌های سه اتمی غیر خطی، بخش 1: H2O (HOH)، بخش ε: HD16O (H16OD)، HT16O (H16OT)، HD17O (H17OD)، HD18O (H18OD)، DT16O (D1)



این زیرجلد داده‌های ارزیابی‌شده را از HD16O، HT16O، HD17O، HD ارائه می‌کند. ایزوتوپولوژی 18O و DT16O. هدف از این مقدمه دسترسی سریعتر به معانی نمادهای موجود در جداول داده است. تئوری ها و معادلات مولکولی را گزارش می کند که بر اساس آنها بیشتر داده های ارزیابی شده در جداول ایجاد شده است. قبل از این جداول یک نمایه اضافی به منظور تسهیل جستجوی اطلاعات خاص وجود دارد.

جدول ها ثابت های مولکولی و/یا کمتر از حدود 5000 سانتی متر–1 را گزارش می کنند که به صورت تجربی تخصیص داده شده اند. موقعیت خط، شدت و پارامترهای مربوط به شکل. منشاء باند ارتعاشی و شدت باند ارتعاشی نیز بدون محدودیت محدوده طیفی ارائه شده است. اطلاعات اضافی (فهرست نمادها با تعاریف آنها، واحدها، جدول ضرایب تبدیل، نمادهای باندها و سطوح انرژی، جداول واحدهای مرتبط با انرژی، ثابت های اساسی انتخاب شده، ...) نیز ارائه شده است. جلد فرعی با یک بخش مرجع به پایان می رسد.


توضیحاتی درمورد کتاب به خارجی

The present subvolume provides evaluated data from HD16O, HT16O, HD17O, HD18O, and DT16O isotopologues. The introduction is intended to give a quicker access to the meanings of symbols found in the data tables. It reports molecular theories and equations, based on which most of the evaluated data given in the tables are established. These tables are preceded by an additional index in order to facilitate the search for specific information.

The tables report molecular constants and/or, below about 5000 cm–1, assigned experimental line positions, intensities, and shape related parameters. Vibrational band origins and vibrational band intensities are also provided with no spectral range limitation. Additional information (list of symbols with their definitions, units, table of conversion factors, notations for the bands and energy levels, tables of energy-related units, selected fundamental constants,…) are also given. The subvolume ends with a reference section.



فهرست مطالب

Front Matter ....Pages i-xiii
 An introduction to the molecular parameters of non-linear triatomic molecules  (G. Guelachvili, N. Picqué)....Pages 1-58
 Molecular constants at ground state of HD16O (H16OD) obtained from spectroscopic method  (G. Guelachvili, N. Picqué)....Pages 59-60
 Molecular constants at ground state of HD16O (H16OD) obtained from microwave spectroscopy  (G. Guelachvili, N. Picqué)....Pages 61-62
 Molecular constants at ground state of HD16O (H16OD) obtained from microwave spectroscopic methods  (G. Guelachvili, N. Picqué)....Pages 63-64
 Molecular constants at ground state of HD16O (H16OD) obtained from microwave spectroscopic methods  (G. Guelachvili, N. Picqué)....Pages 65-65
 Molecular constants of HD16O (H16OD) at (010) state  (G. Guelachvili, N. Picqué)....Pages 66-67
 Molecular constants of HD16O (H16OD) at (100) and (020) states  (G. Guelachvili, N. Picqué)....Pages 68-69
 Fermi and Coriolis coupling constants of HD16O (H16OD) at (100) and (020) states  (G. Guelachvili, N. Picqué)....Pages 70-70
 Molecular constants of HD16O (H16OD) at (110) and (030) states  (G. Guelachvili, N. Picqué)....Pages 71-72
 Fermi and Coriolis coupling constants of HD16O (H16OD) at (110) and (030) states  (G. Guelachvili, N. Picqué)....Pages 73-73
 Molecular constants of HD16O (H16OD) at (001), (110) and (030) states obtained from grating spectroscopy  (G. Guelachvili, N. Picqué)....Pages 74-75
 Fermi coupling constants of HD16O (H16OD) at (110) and (030) states obtained from grating spectroscopy  (G. Guelachvili, N. Picqué)....Pages 76-76
 Molecular constants of HD16O (H16OD) at (001) state  (G. Guelachvili, N. Picqué)....Pages 77-78
 Molecular constants of HD16O (H16OD) at (011), (200), (120) and (040) states  (G. Guelachvili, N. Picqué)....Pages 79-80
 Fermi and Coriolis coupling constants of HD16O (H16OD) at (011), (200), (120) and (040) states  (G. Guelachvili, N. Picqué)....Pages 81-81
 Molecular constants of HD16O (H16OD) at (000), (101), (210), (021), (130) and (050) states  (G. Guelachvili, N. Picqué)....Pages 82-83
 Fermi and Coriolis coupling constants of HD16O (H16OD) at (101), (210), (021), (130) and (050) states  (G. Guelachvili, N. Picqué)....Pages 84-85
 Molecular constants of HD16O (H16OD) at (300), (111), (031) and (060) states  (G. Guelachvili, N. Picqué)....Pages 86-87
 Fermi and Coriolis coupling constants of HD16O (H16OD) at (300), (111), (031) and (060) states  (G. Guelachvili, N. Picqué)....Pages 88-88
 Molecular constants of HD16O (H16OD) at (012) state  (G. Guelachvili, N. Picqué)....Pages 89-90
 Molecular constants of HD16O (H16OD) at (022) and (102) states  (G. Guelachvili, N. Picqué)....Pages 91-92
 Fermi and Coriolis coupling constants of HD16O (H16OD) at (022) and (102) states  (G. Guelachvili, N. Picqué)....Pages 93-93
 Molecular constants of HD16O (H16OD) at (022) and (102) states obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 94-95
 Fermi and Coriolis coupling constants of HD16O (H16OD) at (022) and (102) states obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 96-96
 Molecular constants of HD16O (H16OD) at (003) state  (G. Guelachvili, N. Picqué)....Pages 97-98
 Molecular constants of HD16O (H16OD) at (003) and (005) states obtained from intracavity laser absorption spectroscopy and optoacoustic spectroscopy  (G. Guelachvili, N. Picqué)....Pages 99-100
 Molecular constants of HD16O (H16OD) at (112) and (032) states obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 101-101
 Fermi and Coriolis coupling constants of HD16O (H16OD) at (112) and (032) states obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 102-102
 Molecular constants of HD16O (H16OD) at (500) state obtained from photo-acoustic spectroscopy  (G. Guelachvili, N. Picqué)....Pages 103-103
 Molecular constants of HD16O (H16OD) at (500) state obtained from Fourier transform intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 104-104
 Molecular constants of HD16O (H16OD) at (023), (103), (151) and (260) states obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 105-105
 Fermi and Coriolis coupling constants of HD16O (H16OD) at (023), (103), (151) and (260) states obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 106-106
 Molecular constants of HD16O (H16OD) at (004) state obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 107-108
 Molecular constants of HD16O (H16OD) at (600) state obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 109-109
 Molecular constants of HD16O (H16OD) at (014), (142) and (0 12 0) states obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 110-111
 Fermi and Coriolis coupling constants of HD16O (H16OD) at (014), (142) and (0 12 0) states obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 112-112
 Molecular constants of HD16O (H16OD) at (005) state obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 113-113
 Molecular constants of HD16O (H16OD) at (024), (104) and (501) states obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 114-114
 Fermi and Coriolis coupling constants of HD16O (H16OD) at (024), (104) and (501) states obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 115-115
 Molecular constants of HD16O (H16OD) at (015) state obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 116-116
 Molecular constants of HD16O (H16OD) at (006) and (007) states  (G. Guelachvili, N. Picqué)....Pages 117-118
 Molecular constants of HD16O (H16OD) at (107), (008), (009) and (00 10) states  (G. Guelachvili, N. Picqué)....Pages 119-120
 Effective and equilibrium ground state rotational constants of HD16O (H16OD) obtained from CVROD PES calculations  (G. Guelachvili, N. Picqué)....Pages 121-122
 Rotational constants of HD16O (H16OD) at (006) and (007) states  (G. Guelachvili, N. Picqué)....Pages 123-123
 Vibrational and Fermi resonance constants of HD16O (H16OD)  (G. Guelachvili, N. Picqué)....Pages 124-125
 Calculated spectroscopic constants of HD16O (H16OD) obtained from ab initio calculations  (G. Guelachvili, N. Picqué)....Pages 126-127
 Calculated spectroscopic constants of HD16O (H16OD) obtained from ab initio calculations  (G. Guelachvili, N. Picqué)....Pages 128-129
 Potential Energy Surface at various CC/MBPT models of HD16O (H16OD) obtained from ab initio calculations  (G. Guelachvili, N. Picqué)....Pages 130-131
 Force constants of HD16O (H16OD) at the electronic ground state obtained from ab initio calculations  (G. Guelachvili, N. Picqué)....Pages 132-134
 Force constants derived from potential energy surface of HD16O (H16OD) obtained from ab initio calculations  (G. Guelachvili, N. Picqué)....Pages 135-136
 Vibrational frequencies of HD16O (H16OD) at (000) state from 0.016 to 33.69 cm−1 obtained from tunable far infrared spectroscopy  (G. Guelachvili, N. Picqué)....Pages 137-139
 Spectral line parameters of HD16O (H16OD) at three (000)–(000) transitions from 7.53 to 8.07 cm−1 obtained from microwave spectroscopy  (G. Guelachvili, N. Picqué)....Pages 140-141
 Wavenumbers of HD16O (H16OD) at the (000)–(000) transitions from 20 to 339 cm−1  (G. Guelachvili, N. Picqué)....Pages 142-147
 Wavenumbers of HD16O (H16OD) at the (000)–(000) transitions from 314 to 518 cm−1  (G. Guelachvili, N. Picqué)....Pages 148-151
 Wavenumbers and intensities of HD16O (H16OD) at the (010)–(010) transitions from 413 to 796 cm−1 obtained from emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 152-157
 Wavenumbers and intensities HD16O (H16OD) at the (001)–(001) transitions from 425 to 595 cm−1 of obtained from emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 158-159
 Wavenumbers and intensities of HD16O (H16OD) at the (020)–(020) transitions from 425 to 683 cm−1 obtained from emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 160-162
 Wavenumbers and intensities of HD16O (H16OD) at the (000)–(000) transitions from 449 to 734 cm−1 obtained from emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 163-166
 Spectral line position, intensity and shape parameters of HD16O (H16OD) at the (000)–(000) transitions from 504 to 834 cm−1  (G. Guelachvili, N. Picqué)....Pages 167-170
 Wavenumbers and intensities of HD16O (H16OD) at the (100)–(010) transitions from 1016 to 1715 cm−1 obtained from emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 171-173
 Wavenumbers and intensities of HD16O (H16OD) at the (010)–(000) transitions from 1040 to 1889 cm−1  (G. Guelachvili, N. Picqué)....Pages 174-199
 Spectral line parameters of HD16O (H16OD) at the (010)–(000) transitions from 1176 to 1649 cm−1  (G. Guelachvili, N. Picqué)....Pages 200-211
 Spectral line position, intensity and shape parameters of HD16O (H16OD) at the (010)–(000) transitions from 1206 to 1664 cm−1  (G. Guelachvili, N. Picqué)....Pages 212-218
 Spectral line parameters of HD16O (H16OD) at rovibrational transitions belonging to the (010)–(000) vibrational band from 1206 to 1344 cm−1  (G. Guelachvili, N. Picqué)....Pages 219-220
 Spectral line position, intensity and shape parameters of HD16O (H16OD) at the (100)–(010) transitions from 1231 to 1574 cm−1  (G. Guelachvili, N. Picqué)....Pages 221-222
 Wavenumbers and intensities of HD16O (H16OD) at the (020)–(010) transitions from 1251 to 1695 cm−1 obtained from emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 223-227
 Wavenumbers and intensities of HD16O (H16OD) at the (110)–(100) transitions from 1251 to 1651 cm−1 obtained from emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 228-233
 Wavenumbers and intensities of HD16O (H16OD) at the (010)–(000) transitions from 1253 to 1664 cm−1 obtained using emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 234-237
 Wavenumbers and intensities of HD16O (H16OD) at the (030)–(020) transitions from 1253 to 1649 cm−1 obtained using emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 238-240
 Wavenumbers and intensities of HD16O (H16OD) at the (011)–(001) transitions from 1256 to 1636 cm−1 obtained using emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 241-243
 Spectral line parameters of HD16O (H16OD) at the (010)–(000) transitions in the frequency range 1260–1342 cm−1 obtained from diode laser spectroscopy  (G. Guelachvili, N. Picqué)....Pages 244-245
 Spectral line parameters of HD16O (H16OD) at the (010)–(000) transitions in the frequency range 1288–1497 cm−1 obtained from spectroscopic method  (G. Guelachvili, N. Picqué)....Pages 246-247
 Spectral line position, intensity and shape parameters of HD16O (H16OD) at the (020)–(010) transitions in the frequency range 1300–1498 cm−1  (G. Guelachvili, N. Picqué)....Pages 248-252
 Spectral line parameters of HD16O (H16OD) at the (010)–(000) transitions in the frequency range 1420–1437 cm−1  (G. Guelachvili, N. Picqué)....Pages 253-256
 Wavenumbers and intensities of HD16O (H16OD) at the (001)–(010) transitions from 1995 to 2511 cm−1 obtained using emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 257-259
 Wavenumbers and intensities of HD16O (H16OD) at the (001)–(010) transitions from 2092 to 2488 cm−1 obtained using emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 260-261
 Wavenumbers and intensities of HD16O (H16OD) at the (110)–(010) transitions from 2312 to 2886 cm−1 obtained using emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 262-263
 Wavenumbers and intensities of HD16O (H16OD) at the (100)–(000) transitions from 2337 to 2907 cm−1 obtained using emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 264-267
 Wavenumbers and intensities of HD16O (H16OD) at the (020)–(000) transitions from 2349 to 3018 cm−1 obtained using emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 268-269
 Wavenumbers and intensities of HD16O (H16OD) at the (110)–(010) transitions from 2735 to 2849 cm−1 obtained using emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 270-273
 Wavenumbers and intensities of HD16O (H16OD) at the (030)–(010) transitions from 2337 to 2907 cm−1 obtained using emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 274-276
 Wavenumbers and intensities of HD16O (H16OD) at the (030)–(010) transitions from 2509 to 2895 cm−1 obtained using emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 277-278
 Spectral line position, intensity and shape parameters of HD16O (H16OD) at the (100)–(000) transitions in the frequency range 2564–2858 cm−1  (G. Guelachvili, N. Picqué)....Pages 279-282
 Spectral line parameters of HD16O (H16OD) at the (100)–(000) transitions in the frequency range 2576–2726 cm−1  (G. Guelachvili, N. Picqué)....Pages 283-285
 Spectral line position, intensity and shape parameters of HD16O (H16OD) at the (020)–(000) transitions in the frequency range 2607–3035 cm−1  (G. Guelachvili, N. Picqué)....Pages 286-290
 Wavenumbers and intensities of HD16O (H16OD) at the (011)–(010) transitions from 3037 to 3857 cm−1 obtained using emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 291-294
 Wavenumbers and intensities of HD16O (H16OD) at the (001)–(000) transitions from 3090 to 3854 cm−1 obtained using emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 295-298
 Wavenumbers and intensities of HD16O (H16OD) at the (011)–(010) transitions from 3296 to 3882 cm−1 obtained using emission spectroscopy  (G. Guelachvili, N. Picqué)....Pages 299-301
 Spectral line position, intensity and shape parameters of HD16O (H16OD) at the (001)–(000) transitions from 3528 to 3836 cm−1  (G. Guelachvili, N. Picqué)....Pages 302-306
 Spectral line position, intensity and shape parameters of HD16O (H16OD) at the (110)–(000) transitions from 3967 to 4267 cm−1  (G. Guelachvili, N. Picqué)....Pages 307-311
 Spectral line position, intensity and shape parameters of HD16O (H16OD) at the (030)–(000) transitions from 4022 to 4292 cm−1  (G. Guelachvili, N. Picqué)....Pages 312-314
 Spectral line position and intensity of HD16O (H16OD) at the (110)–(000) transitions from 4201 to 4439 cm−1  (G. Guelachvili, N. Picqué)....Pages 315-318
 Spectral line position, intensity and shape parameters of HD16O (H16OD) at the (110)–(000) transitions from 4201 to 4439 cm−1  (G. Guelachvili, N. Picqué)....Pages 319-322
 Spectral line position and intensity of HD16O (H16OD) at the (030)–(000) transitions from 4202 to 4365 cm−1  (G. Guelachvili, N. Picqué)....Pages 323-325
 Spectral line position, intensity and shape parameters of HD16O (H16OD) at the (030)–(000) transitions from 4202 to 4365 cm−1  (G. Guelachvili, N. Picqué)....Pages 326-328
 Spectral line position, intensity and shape parameters of HD16O (H16OD) at the (011)–(000) transitions from 4960 to 5244 cm−1  (G. Guelachvili, N. Picqué)....Pages 329-333
 Spectral line position and intensity of HD16O (H16OD) at the (011)–(000) transitions from 4960 to 5246 cm−1  (G. Guelachvili, N. Picqué)....Pages 334-337
 Spectral line position, intensity and shape parameters of HD16O (H16OD) at the (011)–(000) transitions from 4960 to 5246 cm−1  (G. Guelachvili, N. Picqué)....Pages 338-341
 Transition moment constants of HD16O (H16OD) at the (010)–(000) transitions  (G. Guelachvili, N. Picqué)....Pages 342-343
 Dipole moment expansion coefficients of HD16O (H16OD) at the (010)–(000) band obtained from spectroscopic method  (G. Guelachvili, N. Picqué)....Pages 344-345
 The air- and self-broadening coefficients of HD16O (H16OD) calculated using semiempirical method  (G. Guelachvili, N. Picqué)....Pages 346-347
 The CO2-broadening coefficients of HD16O (H16OD) calculated using semiempirical method  (G. Guelachvili, N. Picqué)....Pages 348-349
 The N2- and O2-broadening coefficients of HD16O (H16OD) calculated using complex Robert-Bonamy formalism  (G. Guelachvili, N. Picqué)....Pages 350-351
 Band origins of HD16O (H16OD) for 100 vibrational transitions  (G. Guelachvili, N. Picqué)....Pages 352-354
 Vibrational band origins of HD16O (H16OD) at (001)–(000), (110)–(000) and (030)–(000) transitions  (G. Guelachvili, N. Picqué)....Pages 355-355
 Vibrational band origins of HD16O (H16OD) at (101)–(000), (021)–(000) and (210)–(000) transitions  (G. Guelachvili, N. Picqué)....Pages 356-356
 Vibrational band origins of HD16O (H16OD) at (041)–(000) and (070)–(000) transitions  (G. Guelachvili, N. Picqué)....Pages 357-357
 Bond dissociation energies of HD16O (H16OD) obtained from triple resonance vibrational spectroscopy and ab initio calculations  (G. Guelachvili, N. Picqué)....Pages 358-358
 Molecular constants of HT16O (H16OT) at the (000) state obtained from microwave spectroscopy  (G. Guelachvili, N. Picqué)....Pages 359-360
 Molecular constants of HT16O (H16OT) at the (000) and (100) states  (G. Guelachvili, N. Picqué)....Pages 361-362
 Molecular constants of HT16O (H16OT) at the (010) state obtained from tunable diode laser and other spectroscopic methods  (G. Guelachvili, N. Picqué)....Pages 363-364
 Calculated harmonic vibrational frequencies and infrared absorption intensities of HT16O (H16OT) using ab initio calculations  (G. Guelachvili, N. Picqué)....Pages 365-365
 Spectroscopic constants of HT16O (H16OT) using ab initio calculations  (G. Guelachvili, N. Picqué)....Pages 366-367
 Calculated spectroscopic constants of HT16O (H16OT) using ab initio calculation methods  (G. Guelachvili, N. Picqué)....Pages 368-369
 Force constants derived from potential energy surface of HT16O (H16OT) using ab initio calculation method  (G. Guelachvili, N. Picqué)....Pages 370-371
 Spectral line position of HT16O (H16OT) at the (000)–(000) transitions from 0.4 to 23.1 cm−1 obtained from microwave spectroscopy  (G. Guelachvili, N. Picqué)....Pages 372-373
 Spectral line position of HT16O (H16OT) at the (010)–(000) transitions from 1088 to 1263 cm−1  (G. Guelachvili, N. Picqué)....Pages 374-378
 Spectral line position, intensity and shape parameters of HT16O (H16OT) at the (010)–(000) transitions from 1262 to 1384 cm−1 obtained from tunable diode laser spectroscopy  (G. Guelachvili, N. Picqué)....Pages 379-379
 Spectral line position and intensity of HT16O (H16OT) at the (010)–(000) transitions from 1262 to 1384 cm−1 obtained from tunable diode laser spectroscopy  (G. Guelachvili, N. Picqué)....Pages 380-381
 Detectable concentration of HT16O (H16OT) at (010)–(000) transitions from 1262 to 1384 cm−1 obtained from tunable diode laser spectroscopy  (G. Guelachvili, N. Picqué)....Pages 382-382
 Spectral line position of HT16O (H16OT) at the (100)–(000) transitions from 2124 to 2383 cm−1  (G. Guelachvili, N. Picqué)....Pages 383-387
 Vibrational band origins of HD16O (H16OD) at the ν1, ν2, and ν3 vibrational transitions  (G. Guelachvili, N. Picqué)....Pages 388-388
 Estimated vibrational band origins of HD16O (H16OD) at the 2ν3, 2ν1 + 2ν2, and ν1 + ν2 + ν3 vibrational transitions around 7200 cm−1  (G. Guelachvili, N. Picqué)....Pages 389-389
 Molecular constants at the ground state of HD17O (H17OD)  (G. Guelachvili, N. Picqué)....Pages 390-391
 Spectral line position of HD17O (H17OD) at the (000)–(000) transitions from 0.3 to 8.1 cm−1 obtained from microwave spectroscopy  (G. Guelachvili, N. Picqué)....Pages 392-393
 Spectral line position of HD17O (H17OD) at the (100)–(000) transitions from 1118 to 1673 cm−1  (G. Guelachvili, N. Picqué)....Pages 394-402
 Vibrational band origins of HD17O (H17OD) at (010) transitions obtained from measured active rotational-vibrational energy levels protocol  (G. Guelachvili, N. Picqué)....Pages 403-403
 Vibrational band origins of HD17O (H17OD) at (002)–(000), (012)–(000), (101)–(000) and (210)–(000) transitions  (G. Guelachvili, N. Picqué)....Pages 404-404
 Bond dissociation energies of HD17O (H17OD) obtained from triple resonance vibrational spectroscopy and ab initio calculations  (G. Guelachvili, N. Picqué)....Pages 405-405
 Molecular constants at the ground state of HD18O (H18OD)  (G. Guelachvili, N. Picqué)....Pages 406-407
 Molecular constants at the ground state of HD18O (H18OD)  (G. Guelachvili, N. Picqué)....Pages 408-409
 Molecular constants of HD18O (H18OD) at the ground state and seven rovibrational transitions  (G. Guelachvili, N. Picqué)....Pages 410-411
 Molecular constants of HD18O (H18OD) at the (004) state obtained from intracavity laser absorption spectroscopy  (G. Guelachvili, N. Picqué)....Pages 412-412
 Fitted parameters of the effective Hamiltonian of HD18O (H18OD) at (000) and (010) vibrational states  (G. Guelachvili, N. Picqué)....Pages 413-414
 Spectral line position and intensity of HD18O (H18OD) at the (000)–(000) transitions from 0.3 to 219 cm−1  (G. Guelachvili, N. Picqué)....Pages 415-420
 Spectral line position and intensity of HD18O (H18OD) at the (010)–(000) transitions from 1159 to 1663 cm−1  (G. Guelachvili, N. Picqué)....Pages 421-424
 Spectral line position, intensity and shape parameters of HD18O (H18OD) at the (020)–(010) transitions from 1212 to 1448 cm−1  (G. Guelachvili, N. Picqué)....Pages 425-426
 Spectral line position, intensity and shape parameters of HD18O (H18OD) at the (010)–(000) transitions from 1215 to 1609 cm−1  (G. Guelachvili, N. Picqué)....Pages 427-432
 Spectral line position, intensity and shape parameters of HD18O (H18OD) at the (010)–(000) transitions from 1246 to 1564 cm−1  (G. Guelachvili, N. Picqué)....Pages 433-436
 Spectral line position and intensity of HD18O (H18OD) at the (100)–(000) transitions from 2517 to 2921 cm−1  (G. Guelachvili, N. Picqué)....Pages 437-441
 Spectral line position, intensity and shape parameters of HD18O (H18OD) at the (100)–(000) transitions from 2586 to 2812 cm−1  (G. Guelachvili, N. Picqué)....Pages 442-444
 Spectral line position and intensity of HD18O (H18OD) at the (020)–(000) transitions from 2623 to 3017 cm−1  (G. Guelachvili, N. Picqué)....Pages 445-448
 Spectral line position, intensity and shape parameters of HD18O (H18OD) at the (001)–(000) transitions from 3568 to 3824 cm−1  (G. Guelachvili, N. Picqué)....Pages 449-452
 Dipole moment expansion coefficients of HD18O (H18OD) at the (010)–(000) band  (G. Guelachvili, N. Picqué)....Pages 453-454
 Vibrational band origins of HD18O (H18OD) at 14 vibrational transitions obtained from measured active rotational-vibrational energy levels protocol  (G. Guelachvili, N. Picqué)....Pages 455-456
 Vibrational band origins of HD18O (H18OD) at the (002)–(000), (012)–(000), (021)–(000), (031)–(000), (050)–(000), (060)–(000), (101)–(000), (111)–(000), (130)–(000), (210)–(000) and (300)–(000) transitions  (G. Guelachvili, N. Picqué)....Pages 457-457
 Vibrational band origins of HD18O (H18OD) at the (101)–(000), (021)–(000) and (210)–(000) transitions  (G. Guelachvili, N. Picqué)....Pages 458-458
 Band intensity of HD18O (H18OD) at the (050)–(000) and (130)–(000) vibrational transitions from 6495 to 7010 cm−1  (G. Guelachvili, N. Picqué)....Pages 459-459
 Predicted lowest bond dissociation energies of HD18O (H18OD) obtained from triple resonance vibrational spectroscopy and ab initio calculations  (G. Guelachvili, N. Picqué)....Pages 460-460
 Molecular constants of DT16O (D16OT) at the (000) state obtained from microwave spectroscopy  (G. Guelachvili, N. Picqué)....Pages 461-462
 Spectroscopic constants of DT16O (D16OT) obtained from ab initio calculations  (G. Guelachvili, N. Picqué)....Pages 463-464
 Spectroscopic constants of DT16O (D16OT) obtained from ab initio calculations  (G. Guelachvili, N. Picqué)....Pages 465-466
 Harmonic vibrational frequencies and infrared absorption intensities of DT16O (D16OT) obtained from ab initio calculations  (G. Guelachvili, N. Picqué)....Pages 467-467
 Force constants derived from potential energy surface of DT16O (D16OT) obtained from ab initio calculations  (G. Guelachvili, N. Picqué)....Pages 468-469
 Spectral line position of DT16O (D16OT) at the (000)–(000) transitions from 1.7 to 22.6 cm−1 obtained from microwave spectroscopy  (G. Guelachvili, N. Picqué)....Pages 470-471




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تمامی حقوق معنوی و مادی وبسایت متعلق به اینترنشنال لایبرری می باشد
نماد اعتماد الکترونیکی