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Atoms 2017, 5(3), 31; doi:10.3390/atoms5030031

Article
Radiative and Collisional Molecular Data and Virtual Laboratory Astrophysics
Vladimir A. Srećković 1,*Orcid, Ljubinko M. Ignjatović 1, Darko Jevremović 2, Veljko Vujčić 2,3 and Milan S. Dimitrijević 2,4Orcid
1
Institute of Physics, Belgrade University, Pregrevica 118, Zemun, 11080 Belgrade, Serbia
2
Astronomical Observatory, Volgina 7, 11060 Belgrade, Serbia
3
Faculty of Organizational Sciences, University of Belgrade, Jove Ilica 154, 11000 Belgrade, Serbia
4
LERMA, Observatoire de Paris, UMR CNRS 8112, UPMC, 92195 Meudon CEDEX, France
*
Correspondence: Tel.: +381-(0)-11-37-13-000
Academic Editor: Elmar Träbert
Received: 4 September 2017 / Accepted: 13 September 2017 / Published: 19 September 2017

Abstract

:
Spectroscopy has been crucial for our understanding of physical and chemical phenomena. The interpretation of interstellar line spectra with radiative transfer calculations usually requires two kinds of molecular input data: spectroscopic data (such as energy levels, statistical weights, transition probabilities, etc.) and collision data. This contribution describes how such data are collected, stored, and which limitations exist. Also, here we summarize challenges of atomic/molecular databases and point out our experiences, problems, etc., which we are faced with. We present overview of future developments and needs in the areas of radiative transfer and molecular data.
Keywords:
atomic/molecular data; radiative and collisional processes; stars

1. Introduction

Many fields in astronomy such as astrophysics, astrochemistry and astrobiology, depend on data for atomic and molecular (A + M) collision and radiative processes. Among these amount of data collections there are atomic and molecular processes and spectral regions that even today are poorly represented. Therefore, there is an urgent need to collect these data in the databases as well as to develop methods for improving the existing ones. Also, this require a joint effort both of scientists and IT software specialists to develop state-of-the-art infrastructures satisfying their needs, such as Virtual Laboratory [1,2,3].

The Base Astrophysical Targets

Nowadays, the data in in the field of astrophysics modeling are especially important and needed for simulations/calculations. For example the A + M data for hydrogen are important for development of atmosphere models of solar and near solar type stars and for radiative transport investigations as well as an understanding of the kinetics of stellar and other astrophysical plasmas [4,5]. Modern codes for stellar atmosphere modelling, like e.g., PHOENIX (see e.g., [6,7,8]) require the knowledge of atomic data, so that the access to such atomic data, via online databases become very important.
The helium A + M data are of interest particularly for helium-rich white dwarf atmospheres investigations [9,10]. Such data are also important in modelling early Universe chemistry (see the paper of Coppola et al., 2013 [11]). The data for H and some metal atoms like Li, Na, Si are important for the exploring of the geo-cosmical plasmas, the interstellar medium as well as for studies of the early Universe chemistry and for the modelling of stellar and solar atmospheres (see, e.g., [12,13]).
Recently, in the papers [14,15,16,17,18] it has been pointed out that the photodissociation of the diatomic molecular ion in the symmetric and non-symmetric cases, are of astrophysical relevance and could be important in modeling of specific stellar atmosphere layers and they should be included in some chemical models. In the symmetric case, it was considered the processes of molecular ion photodissociation (bound-free) and ion-atom photoassociation (free-bound):
h ν + A 2 + A + A + ,
where A and A + are atom and ion in their ground states, and A 2 + is molecular-ion in the ground electronic state.
In the non-symmetric case, the similar processes of photodissociation/photoassociation are:
h ν + A M + A + + M ,
where M is an atom whose ionization potential is less than the corresponding value for atom A. A M + is also molecular-ion in the ground electronic state.
In the general case molecular ion A 2 + or A M + can be in one of the states from the group which contains the ground electronic state. For the solar atmosphere, A usually denotes atom H(1s) and M one of the relevant metal atoms (Mg, Si, Ca, Na) [14,15,16], but there are cases where A = He, and M = H, Mg, Si, Ca, Na. For the helium-rich white dwarf atmospheres A denotes He(1s 2 ) and M denotes, H(1s), and eventually carbon or oxygen [19,20].
Recently, the results from [16] show the importance of including the symmetric processes with A = H(1s) in the stellar atmosphere models like [5]. Also, for modeling the DB white dwarf atmospheres results for case A = He(1s 2 ) have been used (Koester 2016, private communication). The photodissociation of HeH + has been extensively studied both from a theoretical and experimentalist point of view and inserted in chemical networks describing the formation and destruction of primordial molecules.
It is well known [21] that the chemical composition of the primordial gas consists of electrons and species such as: helium- He, He + , He 2 + and HeH + ; hydrogen- H, H , H + , H 2 + and H 2 ; deuterium- D, D + , HD, H D + and H D ; lithium- Li, Li + , Li , LiH and LiH + . Evaluation of chemical abundances in the standard BB model are calculated from a set of chemical reactions for the early universe [21] and is presented at Figure 1 from [21]. One can see that among them are species like molecular ions H 2 + , H D + , HeH + , etc., whose role in the primordial star formation is important.

2. MolD

2.1. Database Description

MolD database contains cross-sections for photodissociation processes [22], as well as corresponding data on molecular species and molecular state characterisations. MolD project is part of Serbian Virtual Observatory (SerVO)1 and Virtual Atomic and Molecular Data Center (VAMDC)2 (see Figure 2).
MolD application is implemented as a customisation and extension of NodeSoftware provided by VAMDC. It complies to VAMDC interoperability standards and protocols for distributed remote queries. The underlying technology is Python-based, with Django as a Web framework [23], MySQL as a relational database system [24]. The web application runs on Apache web server.
The data model of MolD application is tailored to specifically suit the needs of the theoretical photodissociation data, and yet to easily map onto VAMDC’s standardized XSAMS3 (XML Schema for Atoms, Molecules and Solids format) schema for representation and exchange of atomic and molecular data4.

2.2. Accessing MolD Data

MolD data can be accessed in several ways:
  • Via MolD homepage (http://servo.aob.rs/mold). There is an AJAX-enabled (Asynchronous JavaScript and XML) web form for data querying as well as calculating and plotting average thermal cross sections along available wavelengths for a given temperatiure.
  • Via VAMDC portal (http://portal.vamdc.eu), where one can pose a distributed query to 30 databases across the European scientific institutes.
  • Via standalone applications which support VAMDC-TAP (Table Access Protoco) for data access and tranformation to VAMDC-XSAMS.
During 2017, MolD entered stage 3 of development. Currently, the database includes cross-section data for processes which involve species such as He 2 + , H 2 + , MgH + , HeH + , LiH + , NaH + . These processes are important for exploring of the interstellar medium, the early Universe chemistry as well as the modeling of different stellar and solar atmospheres (see papers [11,15,16,20,22]).
Our plans include transition to new versions of Django framework and NodeSoftware, with ongoing incremental inclusion of A + M data from our papers. We also intend to develop a more intuitive interface for querying and presentation of multidimensional data on our website.

2.3. Example: H 2 + Molecular Ion

MolD is available online from the end of 2014 and it contains the data for the photodissociation processes Equation (1) with A = H(1s) and A = He(1s 2 ). Also it contains the relevant data for some other non-symmetric photodissociation processes Equation (2) where M = Li, Na, Mg or He.
The methods of calculation. The cross-sections for the photodissociation of individual ro-vibrational state of the considered molecular ion H 2 + is determined in the dipole approximation [14]:
σ J , v ( λ ) = 8 π 3 3 λ ( J + 1 ) | D E , J + 1 ; v , J | 2 + J | D E , J 1 ; v , J | 2 2 J + 1 ,
and the corresponding averaged thermal cross sections are given by:
σ phd ( λ , T ) = 1 Z J v g J ; v ( 2 J + 1 ) e E J v E 00 k B T σ J , v ( λ ) .
where T is temperature, λ -wavelength, D E , J + 1 ; v , J is the radial matrix element [25], E J v is the energy of the individual states with the angular and vibrational quantum numbers J and v respectively, and Z is the partition function
Z = J v g J ; v ( 2 J + 1 ) e E J v E 0 , 0 k B T .
In this expression the product g J ; v × ( 2 J + 1 ) is the statistical weight of the considered state and the coefficient g J ; v depends on the “the spin of the nuclei”.
The photo-dissociation crosssection σ p h d ( λ , T ) given by Equation (4), as well as the coefficients K i a ( λ , T ) , are determined within the approximation where the processes are treated as the result of the radiative transitions between the ground and the first excited adiabatic electronic state of the molecular ion H 2 + which are caused by the interaction of the electron component of the ion-atom system with the free electromagnetic field taken in the dipole approximation.
For determination of σ p h d ( λ , T ) , as well as the coefficients K i a ( λ , T ) it is important to know the dipole matrix element D 12 ( R ) defined by relations
D 12 ( R ) = D 12 ( R ) , D 12 ( R ) = 1 | D ( R ) | 2
where R = | R | and D ( R ) is the operator of electron dipole momentum. The mentioned adiabatic electronic states, X 2 g + and A 2 u , are denoted here with | 1 and | 2 and R is the internuclear distance in the considered ion-atom system.
The described mechanism of the processes causes absorption of the photon with energy ϵ λ near the resonant point R = R λ , where R λ is the root of the equation
U 12 ( R ) U 1 ( R ) U 2 ( R ) = ϵ λ .
where U 1 ( R ) corresponds to the ground electronic state, and U 2 ( R ) —to the first excited electronic state.
In Figure 3 are presented the data for σ J , v ( λ ) Equation (3) for the case J = 0 and v = 10 , in the wavelength region 50 nm λ 1500 nm .
The spectral coefficients. The absorption process (1) i.e., processes of molecular ion photodissociation (bound-free) for the case A = H is characterized by partial spectral absorption coefficients κ i a ( λ ) (see e.g., [25]) taken in the form
κ i a ( λ ) = σ p h d ( λ , T ) N ( H 2 + )
where N ( H 2 + ) is density of the H 2 + and σ p h d ( λ , T ) is average cross-section for photo-dissociation of this molecular ion given by Equation (4). As in previous papers [14,25] the partial spectral absorption coefficient κ i a ( λ ) is also used in the form
κ i a ( λ ) = K i a ( λ , T ) N ( H ) N ( H + )
where the coefficient K i a ( λ , T ) is connected with σ p h d ( λ , T ) by the relations
K i a ( λ , T ) = σ p h d ( λ , T ) χ 1 , χ = N ( H ) N ( H + ) N ( H 2 + ) .
In accordance with the definition of the absorption coefficient κ i a ( λ ) , the coefficient K i a ( λ , T ) is given in units (cm 5 ). The results for the average photodissociation cross-section σ p h d ( λ , T ) for H 2 + molecular ion are illustrated by Figure 4. The curves in this figure show the behavior of σ p h d ( λ , T ) as a function of λ for a wide range of temperatures T, which are relevant for the stelar atmosphere (e.g., solar photosphere). The values of the coefficient K i a ( λ , T ) , defined by Equation (10), are presented in the Table 1 for the regions 90 nm λ 370 nm with small wavelength steps and for 3000 K T 10 , 000 K in order to enable easier use (interpolation) of this results. This allows direct calculation of the spectral absorption coefficients during the process of applying a any atmosphere model with the given parameters of plasma and composition.
Solar atmosphere: absorption processes. The influence of radiation processes (1) can bee estimated by comparing their intensities with the intensities of known concurrent radiation processes, namely:
ε λ + H H + e H + e
ε λ + H * H + + e H + + e
The relative contributions of the processes (1), with respect to processes (11) and (12), is described by the quantities F κ defined by relation
F κ = κ i a κ e a + κ e i
where κ e a is absorption spectral coefficient of processes (11) and κ e i is absorption spectral coefficient of processes (12) (see papers [14,16]).
Similarly to the He case in DB white dwarf atmosphere [25] calculations of the absorption coefficient were performed for the solar photosphere and lower chromosphere by means of a standard Solar atmosphere model [5], and the total contribution of the processes (1) to the solar opacity was estimated [16]. The results of the calculations of the parameter F κ for 92 nm λ 350 nm are presented in Figure 5. The figure show that in the significant part of the considered region of altitudes ( 75 km h 1065 km ) the absorption process (1) together give the contribution which varies from about 10 % to about 90 % of the contribution of the absorption process (11) and (12), which are considered as the main absorption processes [16].
On the basis of the above, it can be concluded that photodissociation processes represent important channels for destruction of molecules in lot of astrophysical environments and features of the interacting radiation are important in their spectral analyses.

3. Future Developments and Concluding Remarks

Exploitation the full potential of A + M data and database services is an ongoing challenge in virtual data centers. There are still many limitations and problems that users are facing with such as poor documentation, missing of data evaluation, no open access, etc. The aim of MolD database is to be accessible, and be used by the wider scientific community, through VAMDC and to follow certain protocols and defined rules in order to eliminate such limitations and problems.
The next step of development i.e., the stage three of MolD development will be the implementation of possibility to fit the tabulated data. We plan to develop fitting formulas for photodissociation cross section as the function of the temperature and wavelength. Also, we intend to update the current database with newly calculated/measured data.
The continuation of such developments and services such as constantly updated online A + M database, is crucial in the field of astrophysics and modern physics due to its rapid development and make an immense impact on the way science is done in the developing world.

Acknowledgments

The authors are thankful to the Ministry of Education, Science and Technological Development of the Republic of Serbia for the support of this work within the projects 176002 and III44002. This work has also been supported by the VAMDC (Virtual Atomic and Molecular Data Centre). VAMDC is funded under the Combination of Collaborative Projects and Coordination and Support Actions Funding Scheme of The Seventh Framework Program. We acknowledge the contribution of late A.A. Mihajlov who collected and calculated much of the data that are presented within the MolD database.

Author Contributions

This work is based on the numerous contributions of all the authors.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Evaluation of chemical abundances in the standard Big Bang (BB) model. Vertical axes are the relative abundances and the horizontal axes are relative to the redshift (taken from [21]).
Figure 1. Evaluation of chemical abundances in the standard Big Bang (BB) model. Vertical axes are the relative abundances and the horizontal axes are relative to the redshift (taken from [21]).
Atoms 05 00031 g001
Figure 2. Snapshot from the query page from the Virtual Atomic and Molecular Data Center (VAMDC) portal.
Figure 2. Snapshot from the query page from the Virtual Atomic and Molecular Data Center (VAMDC) portal.
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Figure 3. The behaviour of the cross-section σ J , v ( λ ) Equation (3) for J = 0 and v = 10 , as a function of λ .
Figure 3. The behaviour of the cross-section σ J , v ( λ ) Equation (3) for J = 0 and v = 10 , as a function of λ .
Atoms 05 00031 g003
Figure 4. The behaviour of the averaged cross-section σ p h d ( λ , T ) for photodissociation of the H 2 + molecular ion, as a function of λ and T.
Figure 4. The behaviour of the averaged cross-section σ p h d ( λ , T ) for photodissociation of the H 2 + molecular ion, as a function of λ and T.
Atoms 05 00031 g004
Figure 5. Upper panel: The behavior of the temperature T, N H and N e as a function of height h within the considered part of the solar atmosphere model; lower panel: A surface plot of the quantity F κ = κ i a / ( κ e a + κ e i ) (data taken from [14]) as a function of λ and height h for a model of the solar photosphere [5].
Figure 5. Upper panel: The behavior of the temperature T, N H and N e as a function of height h within the considered part of the solar atmosphere model; lower panel: A surface plot of the quantity F κ = κ i a / ( κ e a + κ e i ) (data taken from [14]) as a function of λ and height h for a model of the solar photosphere [5].
Atoms 05 00031 g005
Table 1. The coefficient K i a ( cm 5 ) Equation (9) as a function of λ and T.
Table 1. The coefficient K i a ( cm 5 ) Equation (9) as a function of λ and T.
λ (nm)3000 K4000 K5000 K6000 K7000 K8000 K9000 K10,000 K
903.50E−372.62E−385.50E−391.93E−399.04E−405.07E−403.20E−402.20E−40
913.75E−372.78E−385.80E−392.03E−399.47E−405.30E−403.34E−402.29E−40
923.99E−372.94E−386.10E−392.12E−399.90E−405.53E−403.48E−402.39E−40
934.23E−373.10E−386.40E−392.22E−391.03E−395.76E−403.62E−402.48E−40
944.47E−373.25E−386.69E−392.31E−391.07E−395.98E−403.76E−402.57E−40
954.71E−373.41E−386.98E−392.41E−391.12E−396.20E−403.89E−402.66E−40
964.95E−373.56E−387.27E−392.50E−391.16E−396.42E−404.03E−402.75E−40
975.18E−373.70E−387.54E−392.59E−391.20E−396.63E−404.16E−402.84E−40
985.40E−373.85E−387.82E−392.68E−391.24E−396.85E−404.29E−402.92E−40
995.62E−373.99E−388.08E−392.76E−391.27E−397.05E−404.41E−403.01E−40
1005.82E−374.12E−388.34E−392.85E−391.31E−397.26E−404.54E−403.09E−40
1016.03E−374.25E−388.59E−392.93E−391.35E−397.46E−404.66E−403.17E−40
1026.22E−374.38E−388.83E−393.01E−391.38E−397.65E−404.78E−403.26E−40
1036.40E−374.50E−389.06E−393.09E−391.42E−397.84E−404.90E−403.34E−40
1046.58E−374.62E−389.29E−393.16E−391.45E−398.03E−405.02E−403.41E−40
1056.74E−374.73E−389.51E−393.24E−391.49E−398.21E−405.13E−403.49E−40
1066.90E−374.83E−389.72E−393.31E−391.52E−398.39E−405.24E−403.57E−40
1077.04E−374.93E−389.92E−393.38E−391.55E−398.57E−405.35E−403.64E−40
1087.18E−375.03E−381.01E−383.44E−391.58E−398.74E−405.46E−403.72E−40
1097.30E−375.11E−381.03E−383.51E−391.61E−398.90E−405.56E−403.79E−40
1107.41E−375.20E−381.05E−383.57E−391.64E−399.06E−405.67E−403.86E−40
1117.52E−375.28E−381.06E−383.62E−391.67E−399.22E−405.77E−403.93E−40
1127.61E−375.35E−381.08E−383.68E−391.69E−399.37E−405.86E−403.99E−40
1137.69E−375.42E−381.09E−383.73E−391.72E−399.52E−405.96E−404.06E−40
1147.77E−375.48E−381.11E−383.79E−391.74E−399.66E−406.05E−404.12E−40
1157.83E−375.54E−381.12E−383.83E−391.77E−399.80E−406.14E−404.18E−40
1167.89E−375.59E−381.13E−383.88E−391.79E−399.93E−406.22E−404.24E−40
1177.93E−375.63E−381.15E−383.93E−391.81E−391.01E−396.31E−404.30E−40
1187.97E−375.68E−381.16E−383.97E−391.83E−391.02E−396.39E−404.36E−40
1198.00E−375.71E−381.17E−384.01E−391.85E−391.03E−396.46E−404.42E−40
1208.02E−375.75E−381.18E−384.05E−391.87E−391.04E−396.54E−404.47E−40
1218.03E−375.78E−381.18E−384.08E−391.89E−391.05E−396.62E−404.52E−40
1228.04E−375.80E−381.19E−384.12E−391.91E−391.06E−396.69E−404.57E−40
1238.04E−375.82E−381.20E−384.15E−391.93E−391.07E−396.76E−404.62E−40
1248.03E−375.84E−381.21E−384.18E−391.94E−391.08E−396.83E−404.67E−40
1258.01E−375.85E−381.21E−384.21E−391.96E−391.09E−396.89E−404.72E−40
1267.99E−375.86E−381.22E−384.23E−391.97E−391.10E−396.96E−404.77E−40
1277.97E−375.87E−381.22E−384.26E−391.99E−391.11E−397.02E−404.81E−40
1287.94E−375.87E−381.23E−384.28E−392.00E−391.12E−397.08E−404.86E−40
1297.90E−375.87E−381.23E−384.30E−392.01E−391.13E−397.14E−404.90E−40
1307.86E−375.87E−381.23E−384.32E−392.03E−391.14E−397.19E−404.94E−40
1317.81E−375.86E−381.24E−384.34E−392.04E−391.15E−397.25E−404.98E−40
1327.76E−375.86E−381.24E−384.36E−392.05E−391.15E−397.30E−405.02E−40
1337.70E−375.84E−381.24E−384.37E−392.06E−391.16E−397.35E−405.06E−40
1347.65E−375.83E−381.24E−384.39E−392.07E−391.17E−397.40E−405.10E−40
1357.58E−375.82E−381.24E−384.40E−392.08E−391.17E−397.45E−405.13E−40
1367.52E−375.80E−381.24E−384.41E−392.09E−391.18E−397.49E−405.17E−40
1377.45E−375.78E−381.24E−384.42E−392.09E−391.19E−397.54E−405.20E−40
1387.38E−375.76E−381.24E−384.43E−392.10E−391.19E−397.58E−405.24E−40
1397.31E−375.73E−381.24E−384.43E−392.11E−391.20E−397.62E−405.27E−40
1407.24E−375.71E−381.24E−384.44E−392.12E−391.20E−397.66E−405.30E−40
1417.16E−375.68E−381.24E−384.45E−392.12E−391.21E−397.70E−405.33E−40
1427.08E−375.65E−381.24E−384.45E−392.13E−391.21E−397.74E−405.36E−40
1437.00E−375.62E−381.23E−384.45E−392.13E−391.22E−397.77E−405.39E−40
1446.92E−375.59E−381.23E−384.46E−392.14E−391.22E−397.80E−405.41E−40
1456.84E−375.56E−381.23E−384.46E−392.14E−391.22E−397.84E−405.44E−40
1466.76E−375.52E−381.23E−384.46E−392.15E−391.23E−397.87E−405.46E−40
1476.68E−375.49E−381.22E−384.46E−392.15E−391.23E−397.90E−405.49E−40
1486.59E−375.45E−381.22E−384.46E−392.15E−391.23E−397.93E−405.51E−40
1496.51E−375.42E−381.22E−384.45E−392.15E−391.24E−397.95E−405.54E−40
1506.42E−375.38E−381.21E−384.45E−392.16E−391.24E−397.98E−405.56E−40
1516.34E−375.34E−381.21E−384.45E−392.16E−391.24E−398.01E−405.58E−40
1526.25E−375.30E−381.20E−384.44E−392.16E−391.25E−398.03E−405.60E−40
1536.17E−375.26E−381.20E−384.44E−392.16E−391.25E−398.05E−405.62E−40
1546.08E−375.22E−381.20E−384.43E−392.16E−391.25E−398.08E−405.64E−40
1556.00E−375.18E−381.19E−384.43E−392.16E−391.25E−398.10E−405.66E−40
1565.91E−375.14E−381.19E−384.42E−392.17E−391.25E−398.12E−405.68E−40
1575.83E−375.10E−381.18E−384.42E−392.17E−391.26E−398.14E−405.70E−40
1585.74E−375.06E−381.18E−384.41E−392.17E−391.26E−398.16E−405.72E−40
1595.66E−375.02E−381.17E−384.40E−392.17E−391.26E−398.18E−405.73E−40
1605.58E−374.98E−381.17E−384.39E−392.17E−391.26E−398.19E−405.75E−40
1625.41E−374.90E−381.16E−384.37E−392.16E−391.26E−398.22E−405.78E−40
1635.33E−374.85E−381.15E−384.36E−392.16E−391.26E−398.24E−405.79E−40
1645.25E−374.81E−381.14E−384.35E−392.16E−391.27E−398.25E−405.81E−40
1655.17E−374.77E−381.14E−384.34E−392.16E−391.27E−398.27E−405.82E−40
1665.09E−374.73E−381.13E−384.33E−392.16E−391.27E−398.28E−405.83E−40
1675.02E−374.68E−381.13E−384.32E−392.16E−391.27E−398.29E−405.85E−40
1684.94E−374.64E−381.12E−384.31E−392.16E−391.27E−398.30E−405.86E−40
1694.86E−374.60E−381.12E−384.30E−392.15E−391.27E−398.31E−405.87E−40
1704.79E−374.56E−381.11E−384.29E−392.15E−391.27E−398.32E−405.88E−40
1714.71E−374.52E−381.10E−384.27E−392.15E−391.27E−398.33E−405.89E−40
1724.64E−374.48E−381.10E−384.26E−392.15E−391.27E−398.34E−405.90E−40
1734.57E−374.43E−381.09E−384.25E−392.14E−391.27E−398.34E−405.91E−40
1744.50E−374.39E−381.09E−384.24E−392.14E−391.27E−398.35E−405.92E−40
1754.43E−374.35E−381.08E−384.22E−392.14E−391.27E−398.36E−405.93E−40
1764.36E−374.31E−381.07E−384.21E−392.13E−391.27E−398.36E−405.94E−40
1774.29E−374.27E−381.07E−384.20E−392.13E−391.27E−398.37E−405.94E−40
1784.22E−374.23E−381.06E−384.18E−392.13E−391.27E−398.37E−405.95E−40
1794.15E−374.19E−381.06E−384.17E−392.12E−391.27E−398.38E−405.96E−40
1804.09E−374.15E−381.05E−384.16E−392.12E−391.27E−398.38E−405.96E−40
1814.02E−374.11E−381.04E−384.14E−392.12E−391.27E−398.38E−405.97E−40
1823.96E−374.07E−381.04E−384.13E−392.11E−391.26E−398.39E−405.98E−40
1833.90E−374.03E−381.03E−384.11E−392.11E−391.26E−398.39E−405.98E−40
1843.84E−374.00E−381.03E−384.10E−392.11E−391.26E−398.39E−405.99E−40
1853.78E−373.96E−381.02E−384.09E−392.10E−391.26E−398.39E−405.99E−40
1863.72E−373.92E−381.01E−384.07E−392.10E−391.26E−398.39E−406.00E−40
1873.66E−373.88E−381.01E−384.06E−392.09E−391.26E−398.39E−406.00E−40
1883.60E−373.84E−381.00E−384.04E−392.09E−391.26E−398.40E−406.01E−40
1893.54E−373.81E−389.95E−394.03E−392.09E−391.26E−398.40E−406.01E−40
1903.49E−373.77E−389.89E−394.01E−392.08E−391.26E−398.40E−406.02E−40
1913.43E−373.73E−389.83E−394.00E−392.08E−391.26E−398.39E−406.02E−40
1923.38E−373.70E−389.77E−393.98E−392.07E−391.26E−398.39E−406.02E−40
1933.33E−373.66E−389.71E−393.97E−392.07E−391.25E−398.39E−406.03E−40
1943.27E−373.63E−389.65E−393.95E−392.06E−391.25E−398.39E−406.03E−40
1953.22E−373.59E−389.59E−393.94E−392.06E−391.25E−398.39E−406.03E−40
1963.17E−373.56E−389.54E−393.92E−392.06E−391.25E−398.39E−406.03E−40
1973.12E−373.52E−389.48E−393.91E−392.05E−391.25E−398.38E−406.04E−40
1983.08E−373.49E−389.42E−393.89E−392.05E−391.25E−398.38E−406.04E−40
1993.03E−373.46E−389.36E−393.88E−392.04E−391.25E−398.38E−406.04E−40
2002.98E−373.42E−389.31E−393.86E−392.04E−391.24E−398.38E−406.04E−40
2052.76E−373.26E−389.03E−393.79E−392.01E−391.24E−398.35E−406.04E−40
2102.56E−373.11E−388.75E−393.71E−391.99E−391.23E−398.33E−406.04E−40
2152.37E−372.97E−388.49E−393.64E−391.96E−391.22E−398.29E−406.03E−40
2202.20E−372.83E−388.24E−393.57E−391.94E−391.21E−398.25E−406.02E−40
2252.04E−372.71E−387.99E−393.50E−391.91E−391.20E−398.21E−406.01E−40
2301.90E−372.59E−387.76E−393.43E−391.89E−391.19E−398.17E−405.99E−40
2351.77E−372.48E−387.53E−393.36E−391.86E−391.18E−398.13E−405.98E−40
2401.66E−372.37E−387.32E−393.30E−391.84E−391.17E−398.08E−405.96E−40
2451.55E−372.27E−387.11E−393.23E−391.81E−391.16E−398.04E−405.94E−40
2501.45E−372.18E−386.92E−393.17E−391.79E−391.15E−397.99E−405.92E−40
2551.36E−372.09E−386.73E−393.11E−391.76E−391.13E−397.94E−405.90E−40
2601.27E−372.01E−386.54E−393.05E−391.74E−391.12E−397.89E−405.87E−40
2651.20E−371.93E−386.37E−392.99E−391.72E−391.11E−397.83E−405.84E−40
2701.12E−371.85E−386.20E−392.94E−391.69E−391.10E−397.78E−405.82E−40
2751.06E−371.78E−386.04E−392.89E−391.67E−391.09E−397.72E−405.79E−40
2809.99E−381.72E−385.89E−392.83E−391.65E−391.08E−397.67E−405.76E−40
2859.43E−381.66E−385.74E−392.78E−391.63E−391.07E−397.62E−405.73E−40
2908.92E−381.60E−385.60E−392.73E−391.61E−391.06E−397.56E−405.70E−40
2958.45E−381.54E−385.47E−392.69E−391.59E−391.05E−397.51E−405.67E−40
3008.00E−381.49E−385.34E−392.64E−391.57E−391.04E−397.46E−405.64E−40
3057.60E−381.44E−385.22E−392.60E−391.55E−391.03E−397.41E−405.61E−40
3107.22E−381.39E−385.10E−392.56E−391.53E−391.02E−397.36E−405.59E−40
3156.86E−381.35E−384.99E−392.52E−391.51E−391.01E−397.32E−405.56E−40
3206.53E−381.31E−384.88E−392.48E−391.49E−391.01E−397.27E−405.53E−40
3256.23E−381.27E−384.78E−392.44E−391.48E−399.96E−407.22E−405.51E−40
3305.94E−381.23E−384.68E−392.40E−391.46E−399.88E−407.17E−405.48E−40
3355.67E−381.19E−384.58E−392.37E−391.44E−399.79E−407.13E−405.45E−40
3405.42E−381.16E−384.49E−392.33E−391.43E−399.71E−407.08E−405.43E−40
3455.19E−381.13E−384.40E−392.30E−391.41E−399.63E−407.04E−405.40E−40
3504.97E−381.09E−384.31E−392.26E−391.40E−399.55E−406.99E−405.37E−40
3554.76E−381.06E−384.23E−392.23E−391.38E−399.47E−406.95E−405.35E−40
3604.57E−381.04E−384.15E−392.20E−391.37E−399.39E−406.90E−405.32E−40
3654.38E−381.01E−384.07E−392.17E−391.35E−399.32E−406.86E−405.29E−40
3704.21E−389.82E−394.00E−392.14E−391.34E−399.24E−406.81E−405.26E−40
Atoms EISSN 2218-2004 Published by MDPI AG, Basel, Switzerland RSS E-Mail Table of Contents Alert
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