Formation of abnormally high density H2S fluid in sedimentary basins
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![]() Figure 1 (a) Occurrences of nodular quartz and calcite cements from the Z1d dolomite at the Caojunba section. (b) A microphoto showing the coexistence of quartz and calcite cements. (c, d) Microphotos showing the petrographic characteristics of typical FIs within the quartz cement. Note that the depth of aqueous inclusions in (c) is different from that for other types of inclusions. | ![]() Figure 2 (a) Raman spectra of gas-liquid-solid three phase and solid-liquid two phase inclusions at room temperature. (b) Raman spectra of gas-liquid two phase inclusions at room temperature. Qz = Quartz; A = Aqueous; V = Vapour; VH2S = Gaseous H2S; LH2S = liquid H2S; SS + H2Sn = Solid S + H2Sn. | ![]() Figure 3 Phase transitions and in situ Raman spectra of three phase inclusions at different temperatures. Phase transition process during heating (a-e) and cooling (f-i). (j) In situ Raman spectra of the solid phase during heating. (k) In situ Raman spectra of the liquid and supercritical phases during heating. LH2S = Liquid H2S; VH2S = Gaseous H2S; SS+H2Sn = Solid S and H2Sn; SM = S melt; SCFH2S = Supercritical H2S; SH2S = Solid H2S; Qz = Quartz. | ![]() Figure 4 A conceptual model describing the formation of high density, high purity H2S fluids. |
Figure 1 | Figure 2 | Figure 3 | Figure 4 |
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Introduction
Mississippi Valley-type (MVT) deposits are among the most significant sedimentary lead-zinc deposits globally, contributing approximately 25 % of the world’s lead-zinc resources (Sośnicka and Lüders, 2019
Sośnicka, M., Lüders, V. (2019) Super-deep, TSR-controlled Phanerozoic MVT type Zn-Pb deposits hosted by Zechstein-2 gas reservoir carbonate (Ca2), Lower Saxony Basin, Germany. Chemical Geology 508, 62–77. https://doi.org/10.1016/j.chemgeo.2018.04.025
). Three metallogenic models are proposed for MVT deposits (Sverjensky, 1981Sverjensky, D.A. (1981) The Origin of a Mississippi Valley-type Deposit in the Viburnum Trend, Southeast Missouri. Economic Geology 76, 1848–1872. https://doi.org/10.2113/gsecongeo.76.7.1848
; Leach et al., 2005Leach, D.L., Sangster, D.F., Kelley, K.D., Large, R.R., Garven, G., Allen, C.R., Gutzmer, J., Walters, S. (2005) Sediment-hosted lead-zinc deposit: a global perspective. In: Hedenquist, J.W., Thompson, J.F.H., Goldfarb, R.J., Richards, J.P. (Eds.) Economic Geology 100th Anniversary Volume, Society of Economic Geologists Inc., USA, 561–607
): the fluid mixing model, the sulfate reduction model and the reduced sulfur model. The former two models are frequently reported to explain the precipitation of galena and sphalerite (Barrie et al., 2009Barrie, C.D., Boyce, A.J., Boyle, A.P., Williams, P.J., Blake, K., Wilkinson, J.J., Lowther, M., McDermott, P., Prior, D.J. (2009) On the growth of colloform textures: A case study of sphalerite from the galmoy ore body, Ireland. Journal of The Geological Society 166, 563–582. https://doi.org/10.1144/0016-76492008-080
; Hurtig et al., 2018Hurtig, N.C., Hanley, J.J., Gysi, A.P. (2018) The role of hydrocarbons in ore formation at the Pillara Mississippi Valley-type Zn-Pb deposit, Canning Basin, Western Australia. Ore Geology Reviews 102, 875–893. https://doi.org/10.1016/j.oregeorev.2018.09.012
; Szmihelsky et al., 2021Szmihelsky, M., Steele-MacInnis, M., Bain, W.M., Falck, H., Adair, R., Campbell, B., Dufrane, S.A., Went, A., Corlett, H.J. (2021) Mixing of brine with oil triggered sphalerite deposition at Pine Point, Northwest Territories, Canada. Geology 49, 488–492. https://doi.org/10.1130/G48259.1
), while the reduced sulfur model is rarely considered (Sverjensky, 1986Sverjensky, D.A. (1986) Genesis of Mississippi Valley-type lead-zinc deposits. Annual Review of Earth and Planetary Sciences 14, 177–199. https://doi.org/10.1146/annurev.ea.14.050186.001141
; Leach et al., 2005Leach, D.L., Sangster, D.F., Kelley, K.D., Large, R.R., Garven, G., Allen, C.R., Gutzmer, J., Walters, S. (2005) Sediment-hosted lead-zinc deposit: a global perspective. In: Hedenquist, J.W., Thompson, J.F.H., Goldfarb, R.J., Richards, J.P. (Eds.) Economic Geology 100th Anniversary Volume, Society of Economic Geologists Inc., USA, 561–607
). The fluid mixing model is particularly effective for rapid formation of MVT deposits (e.g., Barrie et al., 2009Barrie, C.D., Boyce, A.J., Boyle, A.P., Williams, P.J., Blake, K., Wilkinson, J.J., Lowther, M., McDermott, P., Prior, D.J. (2009) On the growth of colloform textures: A case study of sphalerite from the galmoy ore body, Ireland. Journal of The Geological Society 166, 563–582. https://doi.org/10.1144/0016-76492008-080
); but requires substantial amounts of H2S. Therefore, the formation of H2S-rich reservoirs is crucial for controlling the efficiency and scale of MVT mineralisation. Previous studies indicate that at elevated temperatures (e.g., T > 120 °C), thermochemical sulfate reduction (TSR) is the predominant mechanism for producing H2S within the deeper sections of sedimentary basins (Worden et al., 1995Worden, R.H., Smalley, P.C., Oxtoby, N.H. (1995) Gas souring by thermochemical sulfate reduction at 140 °C. AAPG Bulletin 79, 854–863.
; Machel et al., 2001Machel, H.G. (2001) Bacterial and thermochemical sulfate reduction in diagenetic settings—old and new insights. Sedimentary Geology 140, 143–175. https://doi.org/10.1016/S0037-0738(00)00176-7
; Sośnicka and Lüders, 2020Sośnicka, M., Lüders, V. (2020) Fluid inclusion evidence for low-temperature thermochemical sulfate reduction (TSR) of dry coal gas in Upper Permian carbonate reservoirs (Zechstein, Ca2) in the North German Basin. Chemical Geology 534, 119453. https://doi.org/10.1016/j.chemgeo.2019.119453
). TSR thus provides a vital sulfur source for metal sulfide precipitation (Powell and MacQueen, 1984Powell, T.G., MacQueen, R.W. (1984) Precipitation of sulfide ores and organic matter: sulfate reactions at Pine Point, Canada. Science 224, 63–66. https://doi.org/10.1126/science.224.4644.63
; Sośnicka and Lüders, 2019Sośnicka, M., Lüders, V. (2019) Super-deep, TSR-controlled Phanerozoic MVT type Zn-Pb deposits hosted by Zechstein-2 gas reservoir carbonate (Ca2), Lower Saxony Basin, Germany. Chemical Geology 508, 62–77. https://doi.org/10.1016/j.chemgeo.2018.04.025
). However, direct evidence supporting the formation and preservation of H2S-rich reservoirs is still lacking.Fluid inclusions (FIs) are important geological records of ore-forming fluids, yet H2S-rich fluids have been rarely identified in FIs from MVT deposits, with most inclusions composed of CO2 and CH4 in the gas phase (Jones and Kesler, 1992
Jones, H.D., Kesler, S.E. (1992) Fluid inclusion gas chemistry in east Tennessee Mississippi Valley-type districts: Evidence for immiscibility and implications for depositional mechanisms. Geochimica et Cosmochimica Acta 56, 137–154. https://doi.org/10.1016/0016-7037(92)90122-Y
; Conliffe et al., 2013Conliffe, J., Wilton, D.H.C., Blamey, N.J.F., Archibald, S.M. (2013) Paleoproterozoic Mississippi Valley Type Pb–Zn mineralization in the Ramah Group, Northern Labrador: Stable isotope, fluid inclusion and quantitative fluid inclusion gas analyses. Chemical Geology 362, 211–223. https://doi.org/10.1016/j.chemgeo.2013.08.032
). Only a few researchers have reported high density H2S fluids in sedimentary basins (Worden et al., 1995Worden, R.H., Smalley, P.C., Oxtoby, N.H. (1995) Gas souring by thermochemical sulfate reduction at 140 °C. AAPG Bulletin 79, 854–863.
; Sośnicka and Lüders, 2020Sośnicka, M., Lüders, V. (2020) Fluid inclusion evidence for low-temperature thermochemical sulfate reduction (TSR) of dry coal gas in Upper Permian carbonate reservoirs (Zechstein, Ca2) in the North German Basin. Chemical Geology 534, 119453. https://doi.org/10.1016/j.chemgeo.2019.119453
), while systematic experimental validation remains scarce. These fluids might actually be elemental sulfur or dissolved H2S with a Raman peak at 2590 cm−1 (Frezzotti et al., 2012Frezzotti, M.L., Tecce, F., Casagli, A. (2012) Raman spectroscopy for fluid inclusion analysis. Journal of Geochemical Exploration 112, 1–20. https://doi.org/10.1016/j.gexplo.2011.09.009
; Schmidt and Seward, 2017Schmidt, C., Seward, T.M. (2017) Raman spectroscopic quantification of sulfur species in aqueous fluids: Ratios of relative molar scattering factors of raman bands of H2S, HS−, SO2, HSO4−, SO42−, S2O32−, S3− and H2O at ambient conditions and information on changes with pressure and temperature. Chemical Geology 467, 64–75. https://doi.org/10.1016/j.chemgeo.2017.07.022
; Hu et al., 2022Hu, M. Chou, I-M., Wang, R., Shang, L., Chen, C. (2022) High solubility of gold in H2S-H2O ± NaCl fluids at 100–200 MPa and 600–800 °C: A synthetic fluid inclusion study. Geochimica et Cosmochimica Acta 330. https://doi.org/10.1016/j.gca.2022.03.006
). Clearly, more reliable geological evidence is needed to test whether high density H2S fluids can be formed in sedimentary basins and to evaluate the validity of the proposed mineralising mechanisms for MVT deposits.The Ediacaran Doushantuo (Z1d) and Dengying (Z2dn) formations are important host rocks for MVT deposits in the Yangtze Block, South China (Zhang et al., 2022
Zhang, W.-D., Li, B., Lu, A-H., Elatikpo, S.M., Chen, H., Chen, X.-D. (2022) Origin of the Early Cambrian Huayuan carbonate-hosted Zn-Pb orefield, South China: Constraints from sulfide trace elements and sulfur isotopes. Ore Geology Reviews 148, 105044. https://doi.org/10.1016/j.oregeorev.2022.105044
). Here we report the discovery of H2S-rich FIs from the Z1d dolomite at the Caojunba section, South China. This study includes: (1) thorough petrographic observations, in situ Raman spectroscopy and microthermometry, of high purity (∼100 %) and high density (0.68–0.76 g/cm3) H2S FIs are discovered for the first time, (2) the temperature-pressure (T-P) conditions of entrapment (134–158 °C; 50–106 MPa) of the high density H2S fluids are reconstructed, affirming an origin from TSR, and (3) by incorporating previous carbon-oxygen isotope analyses, we propose that calcite precipitation consumes CO2, which in turn purifies H2S within the fluid. In summary, this study presents a new mechanism for the formation of high density, high purity H2S fluids in sedimentary basins, and provides new insights for the precipitation of metal sulfides in MVT deposits.top
Samples and Methods
The Ediacaran strata cover the entire Yangtze Block in South China, including Z1d and Z2dn. The nodular pore-filling quartz-calcite cements are common in the upper Z1d and the lower to middle Z2dn dolomites hosting MVT deposits (e.g., Yangjiaping, Zhongling, Caojunba, Nanbeizhen, and Zouma sections; Shi et al., 2022
Shi, H., Ouyang, Q., Zhou, C., Xiao, S., Chen, Z., Guan, C. (2022) Integrated study of the Doushantuo Formation in northwestern Hunan Province: Implications for Ediacaran chemostratigraphy and biostratigraphy in South China. Precambrian Research 377, 106699. https://doi.org/10.1016/j.precamres.2022.106699
; Cui et al., 2022Cui, H., Kaufman, A.J., Xiao, S., Zhou, C., Zhu, M., Cao, M., Loyd, S., Crockford, P., Liu, X.-M., Goderis, S., Wang, W., Guan, C. (2022) Dynamic interplay of biogeochemical C, S and Ba cycles in response to the Shuram oxygenation event. Journal of The Geological Society 179, jgs2021-81. https://doi.org/10.1144/jgs2021-081
). The studied dolomite and nodular cement samples are collected from the Z1d strata at the Caojunba section (Northwestern Hunan Province, South China), where quartz and calcite nodules commonly occur along the bedding (Shi et al., 2022Shi, H., Ouyang, Q., Zhou, C., Xiao, S., Chen, Z., Guan, C. (2022) Integrated study of the Doushantuo Formation in northwestern Hunan Province: Implications for Ediacaran chemostratigraphy and biostratigraphy in South China. Precambrian Research 377, 106699. https://doi.org/10.1016/j.precamres.2022.106699
; Fig. S-1).The collected rock samples are prepared as doubly polished thin sections for petrographic observations. Compositions of selected FIs are characterised by using Raman spectrometer. Microthermometry and thermodynamic modelling are conducted to reconstruct the FIs trapping T-P conditions. Detailed descriptions of geological settings and methods can be found in the Supplementary Information.
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Results
Petrographic characteristics. There is no obvious cross-cutting relationship between the quartz and calcite cements within the nodules (Fig. 1a,b), indicating that they likely formed contemporaneously. Due to the small size of the FIs in the calcite cement (<5 μm), this study primarily focuses on the petrology, microthermometry, and Raman spectroscopy of quartz cement-hosted FIs. Only a limited number of two phase aqueous inclusions in the calcite cement are subjected to microthermometric analyses. At room temperature, the FIs are classified into three types based on the phase states of their contents: gas-liquid-solid three phase inclusions, gas-liquid two phase inclusions, and solid-liquid two phase inclusions (Fig. 1c,d). Both three phase and solid-liquid two phase inclusions exhibit irregular shapes, with long axes ranging from 5 to 15 μm. The gas-to-liquid ratio in the three phase inclusions varies from 1 to 5 %. These FIs typically occur in clusters or linear arrays. Gas-liquid two phase inclusions also show irregular shapes, with a gas-to-liquid ratio of ∼2 % and a long axis of 3 to 12 μm. They often occur with three phase inclusions (Fig. 1c).

Figure 1 (a) Occurrences of nodular quartz and calcite cements from the Z1d dolomite at the Caojunba section. (b) A microphoto showing the coexistence of quartz and calcite cements. (c, d) Microphotos showing the petrographic characteristics of typical FIs within the quartz cement. Note that the depth of aqueous inclusions in (c) is different from that for other types of inclusions.
Raman spectroscopic characteristics. In three phase inclusions, the typical Raman peaks for the gas and liquid phases appear at ∼2610 cm−1 and ∼2580 cm−1, respectively, with water peaks being nearly undetectable (Fig. 2a). The solid phase exhibits major Raman peaks at ∼221 cm−1, ∼473 cm−1, ∼823 cm−1, ∼873 cm−1, ∼2500 cm−1, and ∼2567 cm−1 (Fig. 2a). In the solid-liquid two phase inclusions, the solid and liquid phases exhibit similar Raman peaks with those observed in the three phase inclusions (Fig. 2a). Gas-liquid two phase inclusions can be further divided into two types based on the liquid phase composition, although they exhibit no obvious difference under the microscope. One type (i) has a liquid phase composed of aqueous solution (3000–3700 cm−1) and dissolved H2S (∼2590 cm−1) and the gas phase exhibits Raman spectral peaks at ∼2610 cm−1 (Fig. 2b). H2S is not identified in the other type (ii) of gas-liquid two phase inclusions (Fig. 2b) which are simple two phase aqueous inclusions (Fig. 2b).

Figure 2 (a) Raman spectra of gas-liquid-solid three phase and solid-liquid two phase inclusions at room temperature. (b) Raman spectra of gas-liquid two phase inclusions at room temperature. Qz = Quartz; A = Aqueous; V = Vapour; VH2S = Gaseous H2S; LH2S = liquid H2S; SS + H2Sn = Solid S + H2Sn.
Microthermometric data. Figure 3a-i presents the phase transition of three phase inclusions during heating and cooling. Upon heating, the volume of the gas bubble gradually decreases, achieving gas-liquid homogenisation (partial homogenisation; L + V > L) at 33 to 57 °C (Fig. 3a-c, Table S-1). As heating continues, the solid components progressively dissolve, resulting in L + V + S > L which produces total homogenisation at temperatures between 113 and 156 °C (Fig. 3d,e, Table S-1). After cooling to room temperature (Fig. 3f), the FIs are cooled to −120 °C, at which point the fluids are completely frozen (Fig. 3g). The freezing of the liquid into a solid can deform the original gas bubble, forming multiple bubbles within the inclusion. Figure 3g shows the formation of a large bubble in the lower right corner and a smaller bubble in the upper left corner of the inclusion. Upon heating, the solid phase begins melting into the liquid phase. For instance, Figure 3h shows that the small bubble in the upper left corner disappears at −86 °C, whereas the larger bubble in the lower right corner remains an irregular shape, indicating incomplete melting of the solid phase. The point at which the bubble transforms from an irregular to a regular spherical shape marks the complete melting of the solid phase (Fig. 3i). This temperature is recorded as the triple point of the fluid within the inclusion (−85.1 to −83.2 °C; Table S-1).

Figure 3 Phase transitions and in situ Raman spectra of three phase inclusions at different temperatures. Phase transition process during heating (a-e) and cooling (f-i). (j) In situ Raman spectra of the solid phase during heating. (k) In situ Raman spectra of the liquid and supercritical phases during heating. LH2S = Liquid H2S; VH2S = Gaseous H2S; SS+H2Sn = Solid S and H2Sn; SM = S melt; SCFH2S = Supercritical H2S; SH2S = Solid H2S; Qz = Quartz.
For the two phase aqueous inclusions, accurately determining the ice melting temperature is challenging due to their small size. As a result, only the Aq + V > Aq homogenisation temperatures are obtained (134–158 °C; Table S-1). By fitting the O-H stretching band of water in the aqueous phase (Wang et al., 2013
Wang, X., Hu, W., Chou, I.-M. (2013) Raman spectroscopic characterization on the OH stretching bands in NaCl–Na2CO3–Na2SO4–CO2–H2O systems: Implications for the measurement of chloride concentrations in fluid inclusions. Journal of Geochemical Exploration 132, 111–119. https://doi.org/10.1016/j.gexplo.2013.06.006
), the chloride concentration is obtained, which ranges from 4.3 to 12.8 wt. % NaCl equiv. Additionally, homogenisation temperatures for a few two phase aqueous inclusions in calcite cement are measured between 138 and 160 °C (Table S-1), which closely align with the homogenisation temperatures of the aqueous inclusions hosted in quartz cement.top
Discussion
Identification of high density H2S inclusions. The 2580 cm−1 and 2610 cm−1 peaks in the three phase inclusions are typical ν1(H2S) vibrational peaks, corresponding to H2S in the liquid and gas phases, respectively (Burke, 2001
Burke, E.A.J. (2001) Raman microspectrometry of fluid inclusions. Lithos 55, 139–158. https://doi.org/10.1016/S0024-4937(00)00043-8
; Frezzotti et al., 2012Frezzotti, M.L., Tecce, F., Casagli, A. (2012) Raman spectroscopy for fluid inclusion analysis. Journal of Geochemical Exploration 112, 1–20. https://doi.org/10.1016/j.gexplo.2011.09.009
; Yu et al., 2021Yu, Y., Hu, W., Chou, I.-M., Jiang, L., Wan, Y., Li, Y., Xin, Y., Wang, X. (2021) Species of Sulfur in Sour Gas Reservoir: Insights from In Situ Raman Spectroscopy of S–H2S–CH4–H2O System and Its Subsystems from 20 to 250°C. Geofluids 2021, 1–14. https://doi.org/10.1155/2021/6658711
; Hu et al., 2022Hu, M. Chou, I-M., Wang, R., Shang, L., Chen, C. (2022) High solubility of gold in H2S-H2O ± NaCl fluids at 100–200 MPa and 600–800 °C: A synthetic fluid inclusion study. Geochimica et Cosmochimica Acta 330. https://doi.org/10.1016/j.gca.2022.03.006
). The three phase inclusions contain minimal to no water, with solid phase Raman peaks at ∼221 cm−1, ∼473 cm−1, ∼823 cm−1, and ∼873 cm−1. These peaks can be attributed to elemental sulfur (i.e. S; Yu et al., 2021Yu, Y., Hu, W., Chou, I.-M., Jiang, L., Wan, Y., Li, Y., Xin, Y., Wang, X. (2021) Species of Sulfur in Sour Gas Reservoir: Insights from In Situ Raman Spectroscopy of S–H2S–CH4–H2O System and Its Subsystems from 20 to 250°C. Geofluids 2021, 1–14. https://doi.org/10.1155/2021/6658711
; Hu et al., 2022Hu, M. Chou, I-M., Wang, R., Shang, L., Chen, C. (2022) High solubility of gold in H2S-H2O ± NaCl fluids at 100–200 MPa and 600–800 °C: A synthetic fluid inclusion study. Geochimica et Cosmochimica Acta 330. https://doi.org/10.1016/j.gca.2022.03.006
). The peak at ∼2500 cm−1 is likely ascribed to polysulfane (H2Sn; Hurai et al., 2019Hurai, V., Černušák, I., Randive, K. (2019) Raman spectroscopic study of polysulfanes (H2Sn) in natural fluid inclusions. Chemical Geology 508, 15–29. https://doi.org/10.1016/j.chemgeo.2018.04.007
), while the ∼2567 cm−1 peak has been hypothesised by Hurai et al. (2019)Hurai, V., Černušák, I., Randive, K. (2019) Raman spectroscopic study of polysulfanes (H2Sn) in natural fluid inclusions. Chemical Geology 508, 15–29. https://doi.org/10.1016/j.chemgeo.2018.04.007
to be H2S bound to crown-shaped cycloocta-sulfur. In two phase inclusions, the Raman peak at ∼2590 cm−1 is assigned to dissolved H2S (Frezzotti et al., 2012Frezzotti, M.L., Tecce, F., Casagli, A. (2012) Raman spectroscopy for fluid inclusion analysis. Journal of Geochemical Exploration 112, 1–20. https://doi.org/10.1016/j.gexplo.2011.09.009
; Schmidt and Seward, 2017Schmidt, C., Seward, T.M. (2017) Raman spectroscopic quantification of sulfur species in aqueous fluids: Ratios of relative molar scattering factors of raman bands of H2S, HS−, SO2, HSO4−, SO42−, S2O32−, S3− and H2O at ambient conditions and information on changes with pressure and temperature. Chemical Geology 467, 64–75. https://doi.org/10.1016/j.chemgeo.2017.07.022
; Hu et al., 2022Hu, M. Chou, I-M., Wang, R., Shang, L., Chen, C. (2022) High solubility of gold in H2S-H2O ± NaCl fluids at 100–200 MPa and 600–800 °C: A synthetic fluid inclusion study. Geochimica et Cosmochimica Acta 330. https://doi.org/10.1016/j.gca.2022.03.006
).In situ Raman spectra of the solid and liquid phases of three phase inclusions are collected during heating (20 °C, 50 °C, 100 °C, and 150 °C; Fig. 3k,j). Previous studies suggest that polysulfane is thermally (e.g., >70 °C) and photochemically sensitive and tends to decompose into hydrogen sulfide and elemental sulfur (H2Sn→(n-1)/8S8 + H2S; Hurai et al., 2019
Hurai, V., Černušák, I., Randive, K. (2019) Raman spectroscopic study of polysulfanes (H2Sn) in natural fluid inclusions. Chemical Geology 508, 15–29. https://doi.org/10.1016/j.chemgeo.2018.04.007
; Hu et al., 2022Hu, M. Chou, I-M., Wang, R., Shang, L., Chen, C. (2022) High solubility of gold in H2S-H2O ± NaCl fluids at 100–200 MPa and 600–800 °C: A synthetic fluid inclusion study. Geochimica et Cosmochimica Acta 330. https://doi.org/10.1016/j.gca.2022.03.006
). This is confirmed by our in situ Raman spectroscopic characterisations. At 100 °C, the polysulfane signal disappears, but elemental sulfur remains detectable in the solid phase (Fig. 3k). With increasing temperature, the Raman peaks of elemental sulfur (∼221 cm−1 and ∼473 cm−1) in the supercritical H2S phase become visible and intensify (Fig. 3j), indicating the progressive dissolution of S in H2S.Volatiles other than the H2S phase (sometimes minor water) at room temperature are not identified in the three phase and solid-liquid two phase inclusions (Fig. 2a), indicating the presence of high purity H2S. Freezing experiments show that the triple points of the volatiles in the three phase inclusions range from −85.1 to −83.2 °C (Table S-1), which is very close to the triple point of pure H2S system (−85.5 °C; Sakoda and Uematsu, 2004
Sakoda, N., Uematsu, M. (2004) A thermodynamic property model for fluid phase hydrogen sulfide. International Journal of Thermophysics 25, 709–737. https://doi.org/10.1023/B:IJOT.0000034234.06341.8a
). Obviously, our microthermometric observations further confirm the presence of high purity H2S. At present, there is no equation of state for the S-H2S system. In addition, the proportion of solid phase in the solid-liquid two phase inclusions is greater than that in the three phase inclusions (Fig. 1c,d). Consequently, three phase inclusions with a lower solid phase proportion (e.g., Fig. 1c) are approximated as pure H2S systems. Based on the homogenisation temperature for liquid and vapour H2S (Lemmon and Span, 2006Lemmon, E.W., Span, R. (2006) Short fundamental equations of state for 20 industrial fluids. Journal of Chemical and Engineering Data 51, 785–850. https://doi.org/10.1021/je050186n
), and the relationship between the ν1(H2S) Raman peak position and H2S density for the homogeneous H2S phase (Jiang et al., 2018Jiang, L., Xin, Y., Chou, I., Chen, Y. (2018) Raman spectroscopic measurements of ν1 band of hydrogen sulfide over a wide range of temperature and density in fused‐silica optical cells. Journal of Raman Spectroscopy 49, 343–350. https://doi.org/10.1002/jrs.5293
), the H2S densities of three phase inclusions are estimated to be 0.68–0.76 g/cm3. Apparently, the investigated inclusions are characterised by high H2S density.The coexistence of three phase inclusions, liquid-solid two phase inclusions, and H2S-bearing two phase aqueous inclusions suggests that the FIs are formed in H2S-saturated immiscible fluid systems (Goldstein, 2001
Goldstein, R.H. (2001) Fluid inclusions in sedimentary and diagenetic systems. Lithos 55, 159–193. https://doi.org/10.1016/S0024-4937(00)00044-X
). Under such circumstances, the homogenisation temperature of the two phase aqueous inclusions can be approximated as their trapping temperature (Goldstein, 2001Goldstein, R.H. (2001) Fluid inclusions in sedimentary and diagenetic systems. Lithos 55, 159–193. https://doi.org/10.1016/S0024-4937(00)00044-X
), which ranges from 134 to 158 °C (Table S-1). By extrapolating along the 0.68–0.76 g/cm3 isochores of the three phase inclusions to 134–158°C yields trapping pressures of 50–106 MPa (Lemmon and Span, 2006Lemmon, E.W., Span, R. (2006) Short fundamental equations of state for 20 industrial fluids. Journal of Chemical and Engineering Data 51, 785–850. https://doi.org/10.1021/je050186n
).Generation of high purity H2S fluid and implications for MVT deposit formation. Previous studies suggest three primary sources of H2S in sedimentary basins: bacterial sulfate reduction (BSR), thermal decomposition of sulfur-bearing compounds, and TSR (Worden et al., 1995
Worden, R.H., Smalley, P.C., Oxtoby, N.H. (1995) Gas souring by thermochemical sulfate reduction at 140 °C. AAPG Bulletin 79, 854–863.
; Sośnicka and Lüders, 2020Sośnicka, M., Lüders, V. (2020) Fluid inclusion evidence for low-temperature thermochemical sulfate reduction (TSR) of dry coal gas in Upper Permian carbonate reservoirs (Zechstein, Ca2) in the North German Basin. Chemical Geology 534, 119453. https://doi.org/10.1016/j.chemgeo.2019.119453
). The sulfur content within the organic matter of these formations is typically limited, resulting in H2S concentrations rarely exceeding 3 % (Machel, 2001Machel, H.G. (2001) Bacterial and thermochemical sulfate reduction in diagenetic settings—old and new insights. Sedimentary Geology 140, 143–175. https://doi.org/10.1016/S0037-0738(00)00176-7
). Cui et al. (2016Cui, H., Xiao, S., Zhou, C., Peng, Y., Kaufman, A.J., Plummer, R.E. (2016) Phosphogenesis associated with the Shuram Excursion: Petrographic and geochemical observations from the Ediacaran Doushantuo Formation of South China. Sedimentary Geology 341, 134–146. https://doi.org/10.1016/j.sedgeo.2016.05.008
, 2017Cui, H., Kaufman, A. J., Xiao, S., Zhou, C., Liu, X.-M. (2017) Was the Ediacaran Shuram Excursion a globally synchronized early diagenetic event? Insights from methane-derived authigenic carbonates in the uppermost Doushantuo Formation, South China. Chemical Geology 450, 59–80. https://doi.org/10.1016/j.chemgeo.2016.12.010
) propose that anaerobic oxidation of methane (AOM) contributes to the formation of 13C-depleted calcite cement (δ13C = −5 ∼ −37 ‰; VPDB). However, our FI observations show that the high density, high purity H2S fluids are generated at 134–158 °C, which exceeds the temperature range conducive to BSR (Machel et al., 2001Machel, H.G. (2001) Bacterial and thermochemical sulfate reduction in diagenetic settings—old and new insights. Sedimentary Geology 140, 143–175. https://doi.org/10.1016/S0037-0738(00)00176-7
). On the contrary, this temperature range aligns with the TSR active range (Machel et al., 2001Machel, H.G. (2001) Bacterial and thermochemical sulfate reduction in diagenetic settings—old and new insights. Sedimentary Geology 140, 143–175. https://doi.org/10.1016/S0037-0738(00)00176-7
; Worden et al., 1995Worden, R.H., Smalley, P.C., Oxtoby, N.H. (1995) Gas souring by thermochemical sulfate reduction at 140 °C. AAPG Bulletin 79, 854–863.
), suggesting that the formation of H2S fluids is more likely attributed to TSR.Detailed petrological observations of the upper Z1d and the lower to middle Z2dn have been conducted by Cui et al. (2016
Cui, H., Xiao, S., Zhou, C., Peng, Y., Kaufman, A.J., Plummer, R.E. (2016) Phosphogenesis associated with the Shuram Excursion: Petrographic and geochemical observations from the Ediacaran Doushantuo Formation of South China. Sedimentary Geology 341, 134–146. https://doi.org/10.1016/j.sedgeo.2016.05.008
, 2017Cui, H., Kaufman, A. J., Xiao, S., Zhou, C., Liu, X.-M. (2017) Was the Ediacaran Shuram Excursion a globally synchronized early diagenetic event? Insights from methane-derived authigenic carbonates in the uppermost Doushantuo Formation, South China. Chemical Geology 450, 59–80. https://doi.org/10.1016/j.chemgeo.2016.12.010
, 2022Cui, H., Kaufman, A.J., Xiao, S., Zhou, C., Zhu, M., Cao, M., Loyd, S., Crockford, P., Liu, X.-M., Goderis, S., Wang, W., Guan, C. (2022) Dynamic interplay of biogeochemical C, S and Ba cycles in response to the Shuram oxygenation event. Journal of The Geological Society 179, jgs2021-81. https://doi.org/10.1144/jgs2021-081
), including outcrops at Zhongling, Yangjiaping and Nanbeizhen (South China), which are only a few kilometres away from the Caojunba section. In the Nanbeizhen section, the nodules are surrounded by finely warping phosphatic dolomite laminations, suggesting that they formed before sediment compaction (Cui et al., 2022Cui, H., Kaufman, A.J., Xiao, S., Zhou, C., Zhu, M., Cao, M., Loyd, S., Crockford, P., Liu, X.-M., Goderis, S., Wang, W., Guan, C. (2022) Dynamic interplay of biogeochemical C, S and Ba cycles in response to the Shuram oxygenation event. Journal of The Geological Society 179, jgs2021-81. https://doi.org/10.1144/jgs2021-081
). Chicken wire and ghost gypsum textures, indicative of original gypsum precipitation characteristic of evaporative environments, are observed within the dolomite sequences (Cui et al., 2022Cui, H., Kaufman, A.J., Xiao, S., Zhou, C., Zhu, M., Cao, M., Loyd, S., Crockford, P., Liu, X.-M., Goderis, S., Wang, W., Guan, C. (2022) Dynamic interplay of biogeochemical C, S and Ba cycles in response to the Shuram oxygenation event. Journal of The Geological Society 179, jgs2021-81. https://doi.org/10.1144/jgs2021-081
). Therefore, we propose that the initial minerals in these nodules are likely evaporites (e.g., gypsum), which provide the sulfates necessary for TSR. The extremely negative δ13Ccarb values (−6.3 to ∼−32.9 ‰, VPDB; Shi et al., 2022Shi, H., Ouyang, Q., Zhou, C., Xiao, S., Chen, Z., Guan, C. (2022) Integrated study of the Doushantuo Formation in northwestern Hunan Province: Implications for Ediacaran chemostratigraphy and biostratigraphy in South China. Precambrian Research 377, 106699. https://doi.org/10.1016/j.precamres.2022.106699
) indicate that carbon in calcite cement is likely of organic origin, possibly involving methane as an electron donor in the TSR process (Cui et al., 2016Cui, H., Xiao, S., Zhou, C., Peng, Y., Kaufman, A.J., Plummer, R.E. (2016) Phosphogenesis associated with the Shuram Excursion: Petrographic and geochemical observations from the Ediacaran Doushantuo Formation of South China. Sedimentary Geology 341, 134–146. https://doi.org/10.1016/j.sedgeo.2016.05.008
). Therefore, TSR is invoked to be responsible for the formation of high density H2S fluids.As shown in Equation 1, TSR not only produces reduced sulfur but also generates CO2 (as HCO3− in the fluid; Worden et al., 1995
Worden, R.H., Smalley, P.C., Oxtoby, N.H. (1995) Gas souring by thermochemical sulfate reduction at 140 °C. AAPG Bulletin 79, 854–863.
; Powell and MacQueen, 1984Powell, T.G., MacQueen, R.W. (1984) Precipitation of sulfide ores and organic matter: sulfate reactions at Pine Point, Canada. Science 224, 63–66. https://doi.org/10.1126/science.224.4644.63
; Sośnicka and Lüders, 2019Sośnicka, M., Lüders, V. (2019) Super-deep, TSR-controlled Phanerozoic MVT type Zn-Pb deposits hosted by Zechstein-2 gas reservoir carbonate (Ca2), Lower Saxony Basin, Germany. Chemical Geology 508, 62–77. https://doi.org/10.1016/j.chemgeo.2018.04.025
).Eq. 1

However, CO2 is absent in the investigated inclusions (Fig. 2). Although the exact formation sequence between calcite and quartz cements is difficult to determine, the homogenisation temperatures of the two phase aqueous inclusions within them are similar (134–158 °C vs. 138–160 °C; Table S-1). Consequently, we tend to conclude that calcite and quartz cements formed in a narrow time range. The sulfates (i.e. gypsum) in the nodules are consumed during the TSR, which generates large amounts of H2S and CO2 (Fig. 4). The latter is consumed through the precipitation of calcite (Eq. 2), which reduces the pore volume and results in the development of a high density (high pressure) H2S fluid.
Eq. 2


Figure 4 A conceptual model describing the formation of high density, high purity H2S fluids.
Obviously, calcite precipitation acts as a sieve, purifying the fluid (i.e. calcite purification model). This also lowers the pH, promoting the precipitation of authigenic silica. By the time quartz precipitates (Eq. 3), CO2 in the fluid has been depleted. As a result,
Eq. 3

H2S and elemental sulfur dissolved in the fluid cannot be incorporated into the calcite lattice and, along with a small amount of water, are trapped as FIs within the quartz crystals.
Both fluid mixing and sulfate reduction are crucial for the formation of MVT deposits (Sverjensky, 1981
Sverjensky, D.A. (1981) The Origin of a Mississippi Valley-type Deposit in the Viburnum Trend, Southeast Missouri. Economic Geology 76, 1848–1872. https://doi.org/10.2113/gsecongeo.76.7.1848
). Our findings are of particular importance to the fluid mixing model. Globally, many MVT deposits exhibit colloform textures in ore minerals such as sphalerite and pyrite, which indicate the rapid precipitation of metal sulfides resulting from the mixing of metal-rich fluids with H2S-rich fluids (Barrie et al., 2009Barrie, C.D., Boyce, A.J., Boyle, A.P., Williams, P.J., Blake, K., Wilkinson, J.J., Lowther, M., McDermott, P., Prior, D.J. (2009) On the growth of colloform textures: A case study of sphalerite from the galmoy ore body, Ireland. Journal of The Geological Society 166, 563–582. https://doi.org/10.1144/0016-76492008-080
). Therefore, an H2S-rich reservoir is essential for the formation of these MVT deposits. This study provides geological evidence that TSR can generate high density H2S fluids and elucidates the important role of TSR in the metallogenic process of MVT deposits, thereby enhancing our understanding of the mineralisation mechanisms of these deposits.top
Conclusions
In the Z1d dolomite at the Caojunba section (South China), high density, high purity H2S inclusions are discovered within nodular quartz cement. Combining petrological, in situ Raman spectroscopic, microthermometric, and previous carbon and oxygen isotope analyses, the following conclusions can be drawn:
- Coexisting vapour and liquid H2S are identified within a single FI at room temperature. The presence of H2S is confirmed by the diagnostic Raman peaks for vapour (∼2610 cm−1) and liquid (∼2580 cm−1) H2S, as well as the measured triple points (−85.1 °C to −83.2 °C). The density of H2S is 0.68–0.76 g/cm3.
- The trapping temperatures of the high density H2S inclusions are concentrated between 134–158 °C. The calcite cement exhibits significantly negative δ13C values, indicating that the high density H2S fluid is formed through TSR. The precipitation of calcite consumes CO2, purifying the fluid and forming a high purity H2S fluid.
- TSR can generate high density, high purity H2S reservoirs, which provide a significant reduced sulfur source for MVT mineralisation.
top
Acknowledgments
This work is supported by the National Natural Science Foundation of China (Grant nos. 42192501, 42173038, 42130109). We thank Qing Ouyang and Zhe Chen for assistance in the fieldwork.
Editor: Rául Fonseca
top
References
Barrie, C.D., Boyce, A.J., Boyle, A.P., Williams, P.J., Blake, K., Wilkinson, J.J., Lowther, M., McDermott, P., Prior, D.J. (2009) On the growth of colloform textures: A case study of sphalerite from the galmoy ore body, Ireland. Journal of The Geological Society 166, 563–582. https://doi.org/10.1144/0016-76492008-080

The former two models are frequently reported to explain the precipitation of galena and sphalerite (Barrie et al., 2009; Hurtig et al., 2018; Szmihelsky et al., 2021), while the reduced sulfur model is rarely considered (Sverjensky, 1986; Leach et al., 2005).
View in article
The fluid mixing model is particularly effective for rapid formation of MVT deposits (e.g., Barrie et al., 2009); but requires substantial amounts of H2S.
View in article
Globally, many MVT deposits exhibit colloform textures in ore minerals such as sphalerite and pyrite, which indicate the rapid precipitation of metal sulfides resulting from the mixing of metal-rich fluids with H2S-rich fluids (Barrie et al., 2009).
View in article
Burke, E.A.J. (2001) Raman microspectrometry of fluid inclusions. Lithos 55, 139–158. https://doi.org/10.1016/S0024-4937(00)00043-8

The 2580 cm−1 and 2610 cm−1 peaks in the three phase inclusions are typical ν1(H2S) vibrational peaks, corresponding to H2S in the liquid and gas phases, respectively (Burke, 2001; Frezzotti et al., 2012; Yu et al., 2021; Hu et al., 2022).
View in article
Conliffe, J., Wilton, D.H.C., Blamey, N.J.F., Archibald, S.M. (2013) Paleoproterozoic Mississippi Valley Type Pb–Zn mineralization in the Ramah Group, Northern Labrador: Stable isotope, fluid inclusion and quantitative fluid inclusion gas analyses. Chemical Geology 362, 211–223. https://doi.org/10.1016/j.chemgeo.2013.08.032

Fluid inclusions (FIs) are important geological records of ore-forming fluids, yet H2S-rich fluids have been rarely identified in FIs from MVT deposits, with most inclusions composed of CO2 and CH4 in the gas phase (Jones and Kesler, 1992; Conliffe et al., 2013).
View in article
Cui, H., Xiao, S., Zhou, C., Peng, Y., Kaufman, A.J., Plummer, R.E. (2016) Phosphogenesis associated with the Shuram Excursion: Petrographic and geochemical observations from the Ediacaran Doushantuo Formation of South China. Sedimentary Geology 341, 134–146. https://doi.org/10.1016/j.sedgeo.2016.05.008

Cui et al. (2016, 2017) propose that anaerobic oxidation of methane (AOM) contributes to the formation of 13C-depleted calcite cement (δ13C = −5 ∼ −37 ‰; VPDB).
View in article
Detailed petrological observations of the upper Z1d and the lower to middle Z2dn have been conducted by Cui et al. (2016, 2017, 2022), including outcrops at Zhongling, Yangjiaping and Nanbeizhen (South China), which are only a few kilometres away from the Caojunba section.
View in article
The extremely negative δ13Ccarb values (−6.3 to ∼−32.9 ‰, VPDB; Shi et al., 2022) indicate that carbon in calcite cement is likely of organic origin, possibly involving methane as an electron donor in the TSR process (Cui et al., 2016).
View in article
Cui, H., Kaufman, A. J., Xiao, S., Zhou, C., Liu, X.-M. (2017) Was the Ediacaran Shuram Excursion a globally synchronized early diagenetic event? Insights from methane-derived authigenic carbonates in the uppermost Doushantuo Formation, South China. Chemical Geology 450, 59–80. https://doi.org/10.1016/j.chemgeo.2016.12.010

Cui et al. (2016, 2017) propose that anaerobic oxidation of methane (AOM) contributes to the formation of 13C-depleted calcite cement (δ13C = −5 ∼ −37 ‰; VPDB).
View in article
Detailed petrological observations of the upper Z1d and the lower to middle Z2dn have been conducted by Cui et al. (2016, 2017, 2022), including outcrops at Zhongling, Yangjiaping and Nanbeizhen (South China), which are only a few kilometres away from the Caojunba section.
View in article
Cui, H., Kaufman, A.J., Xiao, S., Zhou, C., Zhu, M., Cao, M., Loyd, S., Crockford, P., Liu, X.-M., Goderis, S., Wang, W., Guan, C. (2022) Dynamic interplay of biogeochemical C, S and Ba cycles in response to the Shuram oxygenation event. Journal of The Geological Society 179, jgs2021-81. https://doi.org/10.1144/jgs2021-081

The nodular pore-filling quartz-calcite cements are common in the upper Z1d and the lower to middle Z2dn dolomites hosting MVT deposits (e.g., Yangjiaping, Zhongling, Caojunba, Nanbeizhen, and Zouma sections; Shi et al., 2022; Cui et al., 2022).
View in article
Detailed petrological observations of the upper Z1d and the lower to middle Z2dn have been conducted by Cui et al. (2016, 2017, 2022), including outcrops at Zhongling, Yangjiaping and Nanbeizhen (South China), which are only a few kilometres away from the Caojunba section.
View in article
In the Nanbeizhen section, the nodules are surrounded by finely warping phosphatic dolomite laminations, suggesting that they formed before sediment compaction (Cui et al., 2022).
View in article
Chicken wire and ghost gypsum textures, indicative of original gypsum precipitation characteristic of evaporative environments, are observed within the dolomite sequences (Cui et al., 2022).
View in article
Frezzotti, M.L., Tecce, F., Casagli, A. (2012) Raman spectroscopy for fluid inclusion analysis. Journal of Geochemical Exploration 112, 1–20. https://doi.org/10.1016/j.gexplo.2011.09.009

These fluids might actually be elemental sulfur or dissolved H2S with a Raman peak at 2590 cm−1 (Frezzotti et al., 2012; Schmidt and Seward, 2017; Hu et al., 2022).
View in article
The 2580 cm−1 and 2610 cm−1 peaks in the three phase inclusions are typical ν1(H2S) vibrational peaks, corresponding to H2S in the liquid and gas phases, respectively (Burke, 2001; Frezzotti et al., 2012; Yu et al., 2021; Hu et al., 2022).
View in article
In two phase inclusions, the Raman peak at ∼2590 cm−1 is assigned to dissolved H2S (Frezzotti et al., 2012; Schmidt and Seward, 2017; Hu et al., 2022).
View in article
Goldstein, R.H. (2001) Fluid inclusions in sedimentary and diagenetic systems. Lithos 55, 159–193. https://doi.org/10.1016/S0024-4937(00)00044-X

The coexistence of three phase inclusions, liquid-solid two phase inclusions, and H2S-bearing two phase aqueous inclusions suggests that the FIs are formed in H2S-saturated immiscible fluid systems (Goldstein, 2001).
View in article
Under such circumstances, the homogenisation temperature of the two phase aqueous inclusions can be approximated as their trapping temperature (Goldstein, 2001), which ranges from 134 to 158 °C (Table S-1).
View in article
Hu, M. Chou, I-M., Wang, R., Shang, L., Chen, C. (2022) High solubility of gold in H2S-H2O ± NaCl fluids at 100–200 MPa and 600–800 °C: A synthetic fluid inclusion study. Geochimica et Cosmochimica Acta 330. https://doi.org/10.1016/j.gca.2022.03.006

These fluids might actually be elemental sulfur or dissolved H2S with a Raman peak at 2590 cm−1 (Frezzotti et al., 2012; Schmidt and Seward, 2017; Hu et al., 2022).
View in article
The 2580 cm−1 and 2610 cm−1 peaks in the three phase inclusions are typical ν1(H2S) vibrational peaks, corresponding to H2S in the liquid and gas phases, respectively (Burke, 2001; Frezzotti et al., 2012; Yu et al., 2021; Hu et al., 2022).
View in article
The three phase inclusions contain minimal to no water, with solid phase Raman peaks at ∼221 cm−1, ∼473 cm−1, ∼823 cm−1, and ∼873 cm−1. These peaks can be attributed to elemental sulfur (i.e. S; Yu et al., 2021; Hu et al., 2022).
View in article
In two phase inclusions, the Raman peak at ∼2590 cm−1 is assigned to dissolved H2S (Frezzotti et al., 2012; Schmidt and Seward, 2017; Hu et al., 2022).
View in article
Previous studies suggest that polysulfane is thermally (e.g., >70 °C) and photochemically sensitive and tends to decompose into hydrogen sulfide and elemental sulfur (H2Sn→(n-1)/8S8 + H2S; Hurai et al., 2019; Hu et al., 2022).
View in article
Hurai, V., Černušák, I., Randive, K. (2019) Raman spectroscopic study of polysulfanes (H2Sn) in natural fluid inclusions. Chemical Geology 508, 15–29. https://doi.org/10.1016/j.chemgeo.2018.04.007

The peak at ∼2500 cm−1 is likely ascribed to polysulfane (H2Sn; Hurai et al., 2019), while the ∼2567 cm−1 peak has been hypothesised by Hurai et al. (2019) to be H2S bound to crown-shaped cycloocta-sulfur.
View in article
Previous studies suggest that polysulfane is thermally (e.g., >70 °C) and photochemically sensitive and tends to decompose into hydrogen sulfide and elemental sulfur (H2Sn→(n-1)/8S8 + H2S; Hurai et al., 2019; Hu et al., 2022).
View in article
Hurtig, N.C., Hanley, J.J., Gysi, A.P. (2018) The role of hydrocarbons in ore formation at the Pillara Mississippi Valley-type Zn-Pb deposit, Canning Basin, Western Australia. Ore Geology Reviews 102, 875–893. https://doi.org/10.1016/j.oregeorev.2018.09.012

The former two models are frequently reported to explain the precipitation of galena and sphalerite (Barrie et al., 2009; Hurtig et al., 2018; Szmihelsky et al., 2021), while the reduced sulfur model is rarely considered (Sverjensky, 1986; Leach et al., 2005).
View in article
Jiang, L., Xin, Y., Chou, I., Chen, Y. (2018) Raman spectroscopic measurements of ν1 band of hydrogen sulfide over a wide range of temperature and density in fused‐silica optical cells. Journal of Raman Spectroscopy 49, 343–350. https://doi.org/10.1002/jrs.5293

Based on the homogenisation temperature for liquid and vapour H2S (Lemmon and Span, 2006), and the relationship between the ν1(H2S) Raman peak position and H2S density for the homogeneous H2S phase (Jiang et al., 2018), the H2S densities of three phase inclusions are estimated to be 0.68–0.76 g/cm3
View in article
Jones, H.D., Kesler, S.E. (1992) Fluid inclusion gas chemistry in east Tennessee Mississippi Valley-type districts: Evidence for immiscibility and implications for depositional mechanisms. Geochimica et Cosmochimica Acta 56, 137–154. https://doi.org/10.1016/0016-7037(92)90122-Y

Fluid inclusions (FIs) are important geological records of ore-forming fluids, yet H2S-rich fluids have been rarely identified in FIs from MVT deposits, with most inclusions composed of CO2 and CH4 in the gas phase (Jones and Kesler, 1992; Conliffe et al., 2013).
View in article
Leach, D.L., Sangster, D.F., Kelley, K.D., Large, R.R., Garven, G., Allen, C.R., Gutzmer, J., Walters, S. (2005) Sediment-hosted lead-zinc deposit: a global perspective. In: Hedenquist, J.W., Thompson, J.F.H., Goldfarb, R.J., Richards, J.P. (Eds.) Economic Geology 100th Anniversary Volume, Society of Economic Geologists Inc., USA, 561–607.

Three metallogenic models are proposed for MVT deposits (Sverjensky, 1981; Leach et al., 2005): the fluid mixing model, the sulfate reduction model and the reduced sulfur model.
View in article
The former two models are frequently reported to explain the precipitation of galena and sphalerite (Barrie et al., 2009; Hurtig et al., 2018; Szmihelsky et al., 2021), while the reduced sulfur model is rarely considered (Sverjensky, 1986; Leach et al., 2005).
View in article
Lemmon, E.W., Span, R. (2006) Short fundamental equations of state for 20 industrial fluids. Journal of Chemical and Engineering Data 51, 785–850. https://doi.org/10.1021/je050186n

Based on the homogenisation temperature for liquid and vapour H2S (Lemmon and Span, 2006), and the relationship between the ν1(H2S) Raman peak position and H2S density for the homogeneous H2S phase (Jiang et al., 2018), the H2S densities of three phase inclusions are estimated to be 0.68–0.76 g/cm3
View in article
By extrapolating along the 0.68–0.76 g/cm3 isochores of the three phase inclusions to 134–158°C yields trapping pressures of 50–106 MPa (Lemmon and Span, 2006).
View in article
Machel, H.G. (2001) Bacterial and thermochemical sulfate reduction in diagenetic settings—old and new insights. Sedimentary Geology 140, 143–175. https://doi.org/10.1016/S0037-0738(00)00176-7

Therefore, the formation of H2S-rich reservoirs is crucial for controlling the efficiency and scale of MVT mineralisation. Previous studies indicate that at elevated temperatures (e.g., T > 120 °C), thermochemical sulfate reduction (TSR) is the predominant mechanism for producing H2S within the deeper sections of sedimentary basins (Worden et al., 1995; Machel et al., 2001; Sośnicka and Lüders, 2020).
View in article
The sulfur content within the organic matter of these formations is typically limited, resulting in H2S concentrations rarely exceeding 3 % (Machel, 2001).
View in article
However, our FI observations show that the high density, high purity H2S fluids are generated at 134–158 °C, which exceeds the temperature range conducive to BSR (Machel et al., 2001).
View in article
On the contrary, this temperature range aligns with the TSR active range (Machel et al., 2001; Worden et al., 1995), suggesting that the formation of H2S fluids is more likely attributed to TSR.
View in article
Powell, T.G., MacQueen, R.W. (1984) Precipitation of sulfide ores and organic matter: sulfate reactions at Pine Point, Canada. Science 224, 63–66. https://doi.org/10.1126/science.224.4644.63

TSR thus provides a vital sulfur source for metal sulfide precipitation (Powell and MacQueen, 1984; Sośnicka and Lüders, 2019).
View in article
As shown in Equation 1, TSR not only produces reduced sulfur but also generates CO2 (as HCO3 − in the fluid; Worden et al., 1995; Powell and MacQueen, 1984; Sośnicka and Lüders, 2019).
View in article
Sakoda, N., Uematsu, M. (2004) A thermodynamic property model for fluid phase hydrogen sulfide. International Journal of Thermophysics 25, 709–737. https://doi.org/10.1023/B:IJOT.0000034234.06341.8a

Freezing experiments show that the triple points of the volatiles in the three phase inclusions range from −85.1 to −83.2 °C (Table S-1), which is very close to the triple point of pure H2S system (−85.5 °C; Sakoda and Uematsu, 2004).
View in article
Schmidt, C., Seward, T.M. (2017) Raman spectroscopic quantification of sulfur species in aqueous fluids: Ratios of relative molar scattering factors of raman bands of H2S, HS−, SO2, HSO4−, SO42−, S2O32−, S3− and H2O at ambient conditions and information on changes with pressure and temperature. Chemical Geology 467, 64–75. https://doi.org/10.1016/j.chemgeo.2017.07.022

These fluids might actually be elemental sulfur or dissolved H2S with a Raman peak at 2590 cm−1 (Frezzotti et al., 2012; Schmidt and Seward, 2017; Hu et al., 2022).
View in article
In two phase inclusions, the Raman peak at ∼2590 cm−1 is assigned to dissolved H2S (Frezzotti et al., 2012; Schmidt and Seward, 2017; Hu et al., 2022).
View in article
Shi, H., Ouyang, Q., Zhou, C., Xiao, S., Chen, Z., Guan, C. (2022) Integrated study of the Doushantuo Formation in northwestern Hunan Province: Implications for Ediacaran chemostratigraphy and biostratigraphy in South China. Precambrian Research 377, 106699. https://doi.org/10.1016/j.precamres.2022.106699

The nodular pore-filling quartz-calcite cements are common in the upper Z1d and the lower to middle Z2dn dolomites hosting MVT deposits (e.g., Yangjiaping, Zhongling, Caojunba, Nanbeizhen, and Zouma sections; Shi et al., 2022; Cui et al., 2022).
View in article
The studied dolomite and nodular cement samples are collected from the Z1d strata at the Caojunba section (Northwestern Hunan Province, South China), where quartz and calcite nodules commonly occur along the bedding (Shi et al., 2022; Fig. S-1).
View in article
The extremely negative δ13Ccarb values (−6.3 to ∼−32.9 ‰, VPDB; Shi et al., 2022) indicate that carbon in calcite cement is likely of organic origin, possibly involving methane as an electron donor in the TSR process (Cui et al., 2016).
View in article
Sośnicka, M., Lüders, V. (2020) Fluid inclusion evidence for low-temperature thermochemical sulfate reduction (TSR) of dry coal gas in Upper Permian carbonate reservoirs (Zechstein, Ca2) in the North German Basin. Chemical Geology 534, 119453. https://doi.org/10.1016/j.chemgeo.2019.119453

Therefore, the formation of H2S-rich reservoirs is crucial for controlling the efficiency and scale of MVT mineralisation. Previous studies indicate that at elevated temperatures (e.g., T > 120 °C), thermochemical sulfate reduction (TSR) is the predominant mechanism for producing H2S within the deeper sections of sedimentary basins (Worden et al., 1995; Machel et al., 2001; Sośnicka and Lüders, 2020).
View in article
Only a few researchers have reported high density H2S fluids in sedimentary basins (Worden et al., 1995; Sośnicka and Lüders, 2020), while systematic experimental validation remains scarce.
View in article
Previous studies suggest three primary sources of H2S in sedimentary basins: bacterial sulfate reduction (BSR), thermal decomposition of sulfur-bearing compounds, and TSR (Worden et al., 1995; Sośnicka and Lüders, 2020).
View in article
Sośnicka, M., Lüders, V. (2019) Super-deep, TSR-controlled Phanerozoic MVT type Zn-Pb deposits hosted by Zechstein-2 gas reservoir carbonate (Ca2), Lower Saxony Basin, Germany. Chemical Geology 508, 62–77. https://doi.org/10.1016/j.chemgeo.2018.04.025

Mississippi Valley-type (MVT) deposits are among the most significant sedimentary lead-zinc deposits globally, contributing approximately 25 % of the world’s lead-zinc resources (Sośnicka and Lüders, 2019).
View in article
TSR thus provides a vital sulfur source for metal sulfide precipitation (Powell and MacQueen, 1984; Sośnicka and Lüders, 2019).
View in article
As shown in Equation 1, TSR not only produces reduced sulfur but also generates CO2 (as HCO3 − in the fluid; Worden et al., 1995; Powell and MacQueen, 1984; Sośnicka and Lüders, 2019).
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Sverjensky, D.A. (1981) The Origin of a Mississippi Valley-type Deposit in the Viburnum Trend, Southeast Missouri. Economic Geology 76, 1848–1872. https://doi.org/10.2113/gsecongeo.76.7.1848

Three metallogenic models are proposed for MVT deposits (Sverjensky, 1981; Leach et al., 2005): the fluid mixing model, the sulfate reduction model and the reduced sulfur model.
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Both fluid mixing and sulfate reduction are crucial for the formation of MVT deposits (Sverjensky, 1981).
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Sverjensky, D.A. (1986) Genesis of Mississippi Valley-type lead-zinc deposits. Annual Review of Earth and Planetary Sciences 14, 177–199. https://doi.org/10.1146/annurev.ea.14.050186.001141

The former two models are frequently reported to explain the precipitation of galena and sphalerite (Barrie et al., 2009; Hurtig et al., 2018; Szmihelsky et al., 2021), while the reduced sulfur model is rarely considered (Sverjensky, 1986; Leach et al., 2005).
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Szmihelsky, M., Steele-MacInnis, M., Bain, W.M., Falck, H., Adair, R., Campbell, B., Dufrane, S.A., Went, A., Corlett, H.J. (2021) Mixing of brine with oil triggered sphalerite deposition at Pine Point, Northwest Territories, Canada. Geology 49, 488–492. https://doi.org/10.1130/G48259.1

The former two models are frequently reported to explain the precipitation of galena and sphalerite (Barrie et al., 2009; Hurtig et al., 2018; Szmihelsky et al., 2021), while the reduced sulfur model is rarely considered (Sverjensky, 1986; Leach et al., 2005).
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Wang, X., Hu, W., Chou, I.-M. (2013) Raman spectroscopic characterization on the OH stretching bands in NaCl–Na2CO3–Na2SO4–CO2–H2O systems: Implications for the measurement of chloride concentrations in fluid inclusions. Journal of Geochemical Exploration 132, 111–119. https://doi.org/10.1016/j.gexplo.2013.06.006

By fitting the O-H stretching band of water in the aqueous phase (Wang et al., 2013), the chloride concentration is obtained, which ranges from 4.3 to 12.8 wt. % NaCl equiv.
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Worden, R.H., Smalley, P.C., Oxtoby, N.H. (1995) Gas souring by thermochemical sulfate reduction at 140 °C. AAPG Bulletin 79, 854–863.

Therefore, the formation of H2S-rich reservoirs is crucial for controlling the efficiency and scale of MVT mineralisation. Previous studies indicate that at elevated temperatures (e.g., T > 120 °C), thermochemical sulfate reduction (TSR) is the predominant mechanism for producing H2S within the deeper sections of sedimentary basins (Worden et al., 1995; Machel et al., 2001; Sośnicka and Lüders, 2020).
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Only a few researchers have reported high density H2S fluids in sedimentary basins (Worden et al., 1995; Sośnicka and Lüders, 2020), while systematic experimental validation remains scarce.
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Previous studies suggest three primary sources of H2S in sedimentary basins: bacterial sulfate reduction (BSR), thermal decomposition of sulfur-bearing compounds, and TSR (Worden et al., 1995; Sośnicka and Lüders, 2020).
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On the contrary, this temperature range aligns with the TSR active range (Machel et al., 2001; Worden et al., 1995), suggesting that the formation of H2S fluids is more likely attributed to TSR.
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As shown in Equation 1, TSR not only produces reduced sulfur but also generates CO2 (as HCO3 − in the fluid; Worden et al., 1995; Powell and MacQueen, 1984; Sośnicka and Lüders, 2019).
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Yu, Y., Hu, W., Chou, I.-M., Jiang, L., Wan, Y., Li, Y., Xin, Y., Wang, X. (2021) Species of Sulfur in Sour Gas Reservoir: Insights from In Situ Raman Spectroscopy of S–H2S–CH4–H2O System and Its Subsystems from 20 to 250°C. Geofluids 2021, 1–14. https://doi.org/10.1155/2021/6658711

The 2580 cm−1 and 2610 cm−1 peaks in the three phase inclusions are typical ν1(H2S) vibrational peaks, corresponding to H2S in the liquid and gas phases, respectively (Burke, 2001; Frezzotti et al., 2012; Yu et al., 2021; Hu et al., 2022).
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The three phase inclusions contain minimal to no water, with solid phase Raman peaks at ∼221 cm−1, ∼473 cm−1, ∼823 cm−1, and ∼873 cm−1. These peaks can be attributed to elemental sulfur (i.e. S; Yu et al., 2021; Hu et al., 2022).
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Zhang, W.-D., Li, B., Lu, A-H., Elatikpo, S.M., Chen, H., Chen, X.-D. (2022) Origin of the Early Cambrian Huayuan carbonate-hosted Zn-Pb orefield, South China: Constraints from sulfide trace elements and sulfur isotopes. Ore Geology Reviews 148, 105044. https://doi.org/10.1016/j.oregeorev.2022.105044

The Ediacaran Doushantuo (Z1d) and Dengying (Z2dn) formations are important host rocks for MVT deposits in the Yangtze Block, South China (Zhang et al., 2022).
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Supplementary Information
The Supplementary Information includes:
- Geological Setting and Samples
- Methods
- Table S-1
- Figure S-1
- Supplementary Information References
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Figures

Figure 1 (a) Occurrences of nodular quartz and calcite cements from the Z1d dolomite at the Caojunba section. (b) A microphoto showing the coexistence of quartz and calcite cements. (c, d) Microphotos showing the petrographic characteristics of typical FIs within the quartz cement. Note that the depth of aqueous inclusions in (c) is different from that for other types of inclusions.

Figure 2 (a) Raman spectra of gas-liquid-solid three phase and solid-liquid two phase inclusions at room temperature. (b) Raman spectra of gas-liquid two phase inclusions at room temperature. Qz = Quartz; A = Aqueous; V = Vapour; VH2S = Gaseous H2S; LH2S = liquid H2S; SS + H2Sn = Solid S + H2Sn.

Figure 3 Phase transitions and in situ Raman spectra of three phase inclusions at different temperatures. Phase transition process during heating (a-e) and cooling (f-i). (j) In situ Raman spectra of the solid phase during heating. (k) In situ Raman spectra of the liquid and supercritical phases during heating. LH2S = Liquid H2S; VH2S = Gaseous H2S; SS+H2Sn = Solid S and H2Sn; SM = S melt; SCFH2S = Supercritical H2S; SH2S = Solid H2S; Qz = Quartz.

Figure 4 A conceptual model describing the formation of high density, high purity H2S fluids.