Received 3 November 2015; accepted 11 January 2016; published 14 January 2016
Ice cores with their entrapped air inclusions provide records of past changes in atmospheric trace gas composition. Knowledge of the link between snow composition and atmospheric pollutants presented at the time of deposition (aerosol and gas) should serve to reconstruct past atmospheric conditions. Ice core chemical signals depend on the chemical composition of precipitations and the post-depositional processes on the surface snow and inside the ice core. The extent of knowledge on the air-snow transfer function depends on whether the species of interest are gaseous or in the condensed phase, and if they are reversible and/or irreversibly deposited to snow. A priori, this function may vary from one site to another, from one component to another, or according to metereological conditions.
Non-reactive aerosols (e.g. sea-salt, soil dust, sulphur and carbonaceous species) are irreversibly trapped in snow  . Gaseous species have a more complex behaviour than non-reactive aerosols. A few of them, such as methane and carbon dioxide, do not chemically interact with ice, and their past concentrations have been reconstructed by analysing air bubbles trapped in ice cores. Gas concentrations are correlated with climate change deduced from the isotopic composition of the ice core   . However, most gases, such as HCl, HNO3, H2O2, and HCHO, interact with ice and these interactions make their transfer function complex  .
The chemical composition of precipitations depends on atmospheric trace components (gases and aerosol) and in-cloud and below-cloud scavenging processes. In cloud scavenging is related on how hydrometeors (ice crystals, snow, droplets) are formed. This topic is seldom discussed in published papers addressing the relationship between gas and aerosol concentrations in the atmosphere and snow in remote regions  -  . Numerous reconstructions of past atmospheric composition have been made assuming that atmospheric signals are representative and are transferred to and preserved in snow   . Previous discussions on precipitation scavenging in the polar regions have supposed that the processes of aerosol removal are dominated by uptake of the aerosol population as condensation or ice nuclei. For this process, Junge  showed that the concentration of a given element in air should be proportional to its concentration in snowfall. Shaw  examined the size distribution and vertical variation of the total aerosol over the Antarctic ice sheet and calculated that the removal of particles by nucleation of ice crystals constituted 90% of the downward particle flux to the surface over the polar ice sheet. Albeit crude and mainly derived from averaged samples, earlier experimental studies on polar ice sheets   supported Junge’s predictions. However, additional improvements in the chemical analysis and/or interpretation of the results concerning snow and ice have cast doubt on much of the earlier data on Antarctic snow and air composition on which the earlier comparisons are based   .
Several procedures have been adopted to analyse the relationship between the chemical composition of aerosol and snow. Sometimes simultaneous samples of aerosol and snow were collected  -   , at others fresh snow and aerosol were not synchronically sampled   .
The results obtained comparing the chemical composition of aerosol and fresh snow have frequently been contradictory, i.e. concentrations in snow and in air are sometimes related and sometimes not       . Published papers frequently compared ion concentration (soluble and/or insoluble) in snow and aerosol, neglecting to discuss the fact that snow could also scavenge chemical compounds in the gas phase. Therefore, field campaigns designed to measure scavenging coefficients should sample aerosol, gases and fresh snow simultaneously. Even the few measurements showing that signals recorded in snow reflect changes observed in the atmosphere  - cannot be generalized as the results are, strictly speaking, specific to the event considered.
Some models developed for the exchange of energy and chemicals between air and snow  -  . Dominé et al.  attempted to reconstruct past polar atmospheric HCl mixing ratios from ice core analysis concluding that the transfer function could not be described by equilibrium thermodynamics. The transfer of HCl (like gaseous water soluble compounds) involves multiple processes and therefore our understanding of the transfer function is incomplete. For compounds that are mostly in the aerosol phase (e.g. H2SO4), the number of processes involved is smaller, and the difficulties therefore fewer. This paper addresses some of the problems responsible for the complex relationship between ice core chemical signals and atmospheric chemical composition of gases and aerosols in polar areas.
2. Formation of Precipitations in Polar Areas
2.1. Physical and Chemical Processes
Clouds and precipitations play a fundamental role in the removal of atmospheric particles and gases. Wet removal of pollutants (aerosol and gas) from the atmosphere comprises in-cloud and below-cloud scavenging. In-cloud scavenging of aerosol includes contributions from both nucleation and impaction scavenging (inertial impaction, Brownian diffusion, thermophoresis, diffusiophoresis, and electrostatic effects), while below-cloud scavenging includes only impaction.
Precipitations in polar regions are prevalently solid and can form in different ways (Figure 1). Pristine small ice crystals can derive from homogeneous nucleation of super-cooled droplets or heterogeneous nucleation (deposition, condensation, contact and immersion freezing). Ice crystals can subsequently grow through water vapour diffusion, impaction and freezing of super-cooled droplets (riming) and from crystal aggregation.
The riming process becomes efficient only if droplet diameter is larger than 10 µm and crystal diameter is greater than about 50, 150 and 300 μm, when considering dendrites, hexagonal plates and columns, respectively   . Riming is likely to be common during the relatively warm summer season in coastal areas of Antarctica, whereas at the South Pole where temperatures are lower, riming is less likely, i.e. the only growth process is water vapour diffusion  -  .
Warburton and Linkletter  observed that the relative proportion of accretional and diffusional growth found in ice crystals and snowflakes falling to the surface in Antarctica varied with location. At stations near the coast a significantly high proportion of crystals grown by accretion of supercooled droplets (riming) was observed, whereas at the South Pole growth was almost entirely by diffusion. Microphysical observations of cloud parameters in the Antarctic show predominantly ice crystal clouds across the interior, with mixed-phase clouds close to the coast  . In the Arctic (northern coast of Alaska), Mossop et al.  and Jayaweera and Ohtake  investigated the microphysical characteristics of arctic stratus clouds, observing no riming process in these clouds. Instead, Asuma et al.  observed both densely rimed dendrites and graupels in the western Canadian Arctic together with crystals grown by diffusion (plates, columns, bullet rosettes). These two different growth
Figure 1. The main processes influencing the chemical composition of snow crystals in Antarctic cloud.
processes influence the amounts and composition of impurities incorporated into hydrometeors and hence in the polar ice sheets.
Few papers on polar areas have reported the concentrations of pollutants considering the different kinds of precipitations separately. For instance, Douglas et al.  collected snow and ice crystals in the air, on the ground and on sea-ice in Alaska to study the deposition of mercury, predominantly present in the atmosphere as a gaseous element. Their results showed that mercury concentrations were related to the type and formation of snow and ice crystals. The concentration of mercury decreased from rime, diamond dust (clear sky precipitations) and surface hoar.
2.2. Gas Scavenging
Considering gas scavenging, the main gases present in the Antarctic atmosphere (SO2, HCl, HNO3, NH3) are highly soluble in water, and therefore in liquid or mixed clouds they are mainly partitioned into supercooled water droplets. The transfer function of such water-soluble trace gases depends on their fate during freezing, which can be split into: 1) non-rime freezing (homogeneous or heterogeneous nucleation) and 2) riming freezing (aggregation of supercooled water droplets with ice hydrometeors). As gases are less soluble in ice than in water, freezing leads to their exclusion from the forming ice. The subsequent increase in gas concentration in the unfrozen fraction water can eventually determine an outgassing to the atmosphere. The overall process is quantified by the retention coefficient, which is the ratio of the solute mass in the hydrometeors after freezing to the mass originally dissolved in the unfrozen droplets. Measured retention coefficients for gases range from 0.01 to 1 and the values depend on the characteristics and concentration of solutes, droplet sizes, riming conditions (dry or wet) and droplet supercooling. Values increase by raising the effective Henry’s constant, i.e. for dissociated soluble gas both in the case of non-rime and riming freezing  .
Published papers report discrepancies in gas retention coefficient values. For SO2, Lamb and Blumenstein  used droplets in the range of a few to 10 μm, measuring an entrapped fraction that was strongly temperature dependent and varied from about 0.01 near 0˚C to more than 0.12 at −20˚C. Iribarne et al.  reported an average value of 0.62, regardless of temperature and SO2 gas phase concentration, for drops ranging from 5 to 40 μm. Santachiara et al.  (1992) showed that gaseous entrapment is greater the higher the freezing rate and increases the lower the SO2 gas concentration.
For HCl, HNO3 and NH3, the retention coefficients measured in laboratory and in-cloud field campaigns are almost unitary  -  . Field measurements of hydrogen peroxide suggest values from 0.05  to 0.24  , widely different from those reported in the laboratory experiments of Iribarne and Pyshnov  , and Blohn et al.  who measured a unitary and 0.64 retention coefficient, respectively. Values of pH, temperature, and drop size varied between and within the studies. In addition to droplet partitioning during freezing, the interaction of trace gases with the ice surface must be considered in order to evaluate the transfer of gases from air to hydrometeors. The interaction of gases with ice is a complex problem and needs to be addressed to reconstruct past atmospheric concentration from ice core analyses.
Here we summarize the main points. By considering non-growing crystals, the trace gases/ice surface interaction occurs through adsorption and diffusion into the bulk crystal. Thermodynamic equilibrium between gas and ice in the adsorption process develops over long time-scales as diffusion coefficients in solids are very small. For instance, the diffusion coefficient of HCl at T = 258 K is about 10 - 12 cm2∙s−1, while that of HNO3 is higher by a factor of about 100  . In addition, HNO3 is about 25 times less soluble in ice than HCl. Therefore, surface adsorption is valid in the atmospheric processes, while diffusion in the bulk should be negligible. For instance, the migration distance of in ice should be about 0.8 cm after 1000 years  .
Laboratory experiments performed in conditions of growing and non-growing crystals in the presence of SO2, HNO3, HCl, NH3 show that gas uptake is higher in the condition of growth   -  . Hoog et al.  showed that non-growing crystals had an NH3 uptake approximately one order of magnitude lower than growing crystals. Published papers prevalently show that crystal uptake of gases increases with the rising gas concentration in air and depends on temperature.
Considering growing ice, several possible mechanisms for the sorption of gases should be considered including surface adsorption and diffusion in the bulk forming a solid solution, co-condensation of gaseous species (i.e. simultaneous condensation of trace gases and water vapour on the ice surface), and dissolution into the quasi-liquid layer (QLL). The impact of QLL should increase by raising the temperature  . Abbatt et al.  measured an enhanced uptake for benzene and acetone at high temperature. QLL thickness strongly depends on temperature and the ionic content of ice  -  . If crystal growth is due to a diffusion process, the mass flux density of the water vapour and trace gases does not depend only on their gradients, but also on a convective or macroscopic flow, known as Stefan flow  -  .
We will focus on the scavenging processes involving (particulate and gaseous) as nitrate is the final product of the oxidation of nitrogen oxides (NOx = NO + NO2) in the atmosphere and one of the anions dominating the chemical composition of the polar snowpack. The NOx cycle is strongly coupled with OH and O3 chemistry in the atmosphere  . Wet and dry deposition of nitrate (as HNO3 or) is a sink for NOx.
By considering the behaviour of nitric acid in the case of non-growing ice, laboratory experiments disclosed a largely irreversible uptake of molecules on a short time-scale   -  . The results, interpreted as ice surface adsorption, are related to the ability of cirrus clouds to scavenge gas-phase HNO3 in the free troposphere. For diffusionally growing ice crystals, laboratory studies indicate a significantly enhanced uptake of nitric acid compared to experiments with an ice film at equilibrium. The uptake is substantially higher than the thermodynamic solubility limit that is established over long time-scales by diffusion and solubility of HNO3 in bulk ice  . Therefore, the uptake of nitric acid molecules on growing ice surfaces leads to more efficient uptake than a pure adsorption and diffusion process     . Several uptake mechanisms were considered in published papers, depending on temperature and HNO3 partial pressure, adsorption onto the surface and formation of a monolayer or multilayer of HNO3 molecules on the ice surface, or co-deposition with water vapour in the growing crystal   . If the snow crystal has a disordered surface layer (liquid-like layer or premelted layer), HNO3 may partition from the gas-phase into the aqueous surface region, governed by an appropriate Henry’s law equilibrium  . Under low-temperature conditions and high partial pressure of HNO3, the ice surface can melt due to melting point depression and a supercooled liquid solution is formed. This solution layer should not be confused with the thin liquid-like layer that exists on the surface of pure ice. In this condition a large uptake of HNO3 can occur. For this reason, the various interactions of HNO3 with ice must be studied to reconstruct past atmospheric HNO3 concentrations from ice core analyses.
Zondlo et al.  observed two different HNO3 uptake regimes. For H2O/HNO3 partial pressure below the supercooled H2O/HNO3 liquid isotherm, a time-dependent uptake of HNO3 was observed until the HNO3 surface coverage reached one monolayer. By contrast, when H2O and HNO3 partial pressures were greater than the supercooled H2O/HNO3 liquid isotherm, a continuous growth was observed. Dominé and Thibert  suggested that HNO3 is incorporated in ice growing by deposition of layers of a given thickness whose composition is determined by condensation kinetics. Solid diffusion is not a viable explanation for the large uptake of HNO3, due to its low diffusion coefficient and solubility in ice  .
By considering HNO3 concentration in sampled snow, a high uptake of gaseous HNO3 in deposited snow sampled at high altitude has been confirmed by experimental field measurements all over the world      -  . Puxbaum and Tscherwenka  collected snow and rime samples at the Sonnblick Observatory (3106 m a.s.l) estimating that more than 35% of in fallen snow came from direct-gas phase scavenging by ice crystals. Mitchell and Lamb  , Mitchell and Borys  , and Duncan  found comparable values of in rimed and unrimed snow. Field measurements disclosed a weak correlation between nitrate in aerosol and snow    and a positive correlation for NO-3in fresh snow, and the sum of HNO3 and nitrate in air    .
3. The Post-Depositional Process
Many post-depositional processes affect the composition of glacial ice. Figure 2 shows some of the post-depo- sitional processes, co-condensation of water vapour and gases with formation of hoar frost on the ice surface, formation of rime on the snow surface during fog episodes, adsorption/desorption of gases, diffusion through the snow/firn layer, an advective process due to wind-pumping, sublimation of snow, volatilization of chemical species, snow grain metamorphism within the pack, chemical and photochemical reactions in snow, and dry deposition. These processes affect and continuously alter the chemical composition of the snow surface, firn, and ice core, and therefore the actual air-to-snow transfer function. Diurnal variations of meteorological parameters (e.g. temperature, water vapour partial pressure, intensity of solar radiation) are closely linked to these processes  .
Figure 2. Scheme of post-depositional processes (adapted from Tranter and Jones  ).
Dry deposition occurs continuously by sedimentation, diffusion, and impaction of particles on the snow surface  . Strong temperature inversions can favour deposition due to thermophoresis. The contribution of dry deposition in Antarctica is higher during winter (due to the lower precipitation rate and decreased scavenging efficiency of unrimed snow in winter), and on sites in central Antarctica, which have very low snow accumulation rates with respect to coastal regions   . According to Gjessing  , dry deposition is the dominant sink on the Antarctic Plateau, whereas snow scavenging predominates in the coastal areas of Antarctica  .
Hoar on snow can form by the deposition of atmospheric vapour water when its surface cools radiatively in the absence of strong winds. Hoar can form even during the day around noon, when the upward flux of water vapour from the warmer snowpack condenses at snowpack surface.
Post-depositional processes include adsorption and desorption of gases from the snow surface. Laboratory results on the adsorption-desorption of gases (e.g. HCl, HNO3, SO2, NH3, H2O2, HCHO, HONO) from non-growing crystals can be assumed to be valid even for surface snow in stationary conditions      -  . Prevalently laboratory results showed a gas uptake decreasing at lower temperatures and a maximum uptake at temperatures near 0˚C, due to the presence of a quasi-liquid layer on the grain surface.
Gases can influence each other during uptake. Runs made with NH3 in the presence of SO2 yielded higher concentrations in the ice phase than did runs made with single gases   ; likewise, SO2 in the presence of oxidants  . Co-adsorption of HCl and HNO3 shows that HNO3 adsorbs more strongly than HCl, and that HCl is displaced from the ice surface as a result of acidification by HNO3  . The presence of an acidic surface (e.g. by the presence of sulphuric acid) can inhibit the uptake of nitric acid  . Sublimation of water vapour from the snow surface of non-volatile compounds can determine an increase in chemical concentration in surface snow records. This could be misinterpreted as dry deposition  .
Metamorphic processes, i.e. changes in the shapes and sizes of snow grains, occur in deposited snow. Grain coarsening was observed in stratigraphy performed by Gow  at the South Pole. Snow ageing reduces the sur- face free energy as grain growth and the surface area decreases, thereby decreasing the potential for surface storage. Metamorphism also affects macroscopic physical properties such as density, thermal conductivity and albedo  -  . A decrease of the snow surface area will result in the emission of trace gases from the snow surface  . Physiochemical and photochemical processes in the snow pack occur for a variety of important chemical species. Surface snow is a porous medium with a high surface area and low density (in the range 0.01 to 0.2 g∙cm−3), and therefore consists prevalently of air. Light can penetrate the surface and the photochemical activity releases gases into the atmosphere (NOx, H2O2, HCHO, organic acid, halogens, etc.). Many studies have observed significant changes in the concentration of gases contained in the deposited snow due to metamorphism, photolysis, diffusion out of the snow crystals, etc.  -  In addition, the distribution of impurities between the different domains of the condensed phase inside the snowpack (at the grain surface, in the bulk of the solid, in liquid trapped in confined pockets between grains), the presence of a multiphase system where liquid solutions and ice coexist, and changes in snow structure and properties affect both physical processes and chemical reactivity  .
Nitrate in Snow, Hoar Surface Crystals and Firn
Nitrate has been measured extensively in ice cores, and advocated as a proxy for a host of different parameters (e.g. lightning frequency, past solar activity, stratospheric temperature). The study of polar ice cores can provide information on sources of NOx (e.g. surface, tropospheric, middle atmospheric sources). Nitrate has traditionally been assumed to be oxidized irreversibly in the atmosphere, and therefore nitrate concentration profiles in ice cores have long been thought to preserve information on atmospheric NOx concentrations. However, more recent studies  -  indicate that the snowpack is reactivating, and it is now acknowledged that its deposition is reversible. Therefore, the link between the atmospheric concentration of NOx and in the ice core is particularly problematic.
Udisti et al.  collected atmospheric aerosol, superficial snow layers and firn samples from snow pits at Dome Concordia station during the 2000/2001 summer field season. Comparative analysis of aerosol, surface hoar and surface snow showed differences in chemical composition. Nitrate and chloride exhibited higher concentrations in the surface hoar with respect to snow samples, and low concentrations were measured in the aerosol. Udisti et al.’s results (2004) demonstrate that nitrate and chloride are mainly in the gas phase at Dome C and can be captured by the snow and hoar surface through dry deposition and adsorption. However, the wet deposition process in polar regions includes precipitations from clouds, clear-sky precipitations, formation of surface hoar frost (prevalently during night-time), and surface deposition of freezing droplets (rime). Therefore, the difference between nitrate/chloride concentrations in hoar frost and snow could also depend on: 1) different scavenging mechanisms for precipitating crystals from clouds and crystals forming near the surface, and 2) a different near-surface gas/aerosol concentration with respect to cloud. An additional interpretation of the high concentrations in “hoar samples” could be the presence of small rime droplets due to fog deposition, highly concentrated in HNO3 almost completely retained during freezing  .
During a campaign carried out at Dome C (January 2009-January 2010), Erbland et al.  compared the particulate nitrate and gaseous HNO3 in the atmosphere with the nitrate concentration of surface snow samples (referred to as the “skin layer”) collected every three days. mass fractions in skin layer snow exhibited a seasonal pattern similar to that observed for the atmosphere, but temporal variations of mass in the skin layer were offset from those observed in the atmosphere by a period of about three to four weeks. In our opinion, the paper suffers from the lack of information on the wet deposition (clouds or cloudless precipitation, hoar formation, surface riming) during the atmospheric and snow samplings in order to explain the results.
Neubauer and Heumann   found much higher nitrate concentrations in hoar frost (548 ng∙g−1) with respect to fresh snow and firn cores (206 ng∙g−1 and 61 ng∙g−1, respectively) in samples collected at the German Antarctic station “Georg-von-Neumayer” (January and February 1987). As snow was collected a few hours after snowfall, the higher concentration in surface hoar should not depend on a photochemistry loss in snow.
Champollion et al.  investigated hoar evolution through continuous observations of the surface by in situ near-infrared photography and passive microwave remote sensing at Dome C. Observations during 18 months even during the polar winter (when the air and snow temperatures are low and air contains very little water vapour) demonstrated that hoar is far from a marginal phenomenon at Dome C. Hoar is present on the surface almost half of the time all year round, and the hoar periods are usually longer in summer than in winter. According to the authors, the nature of these crystals is either “surface hoar” formed by condensation of the air water vapour onto the surface during the night, or frost flower-like crystals formed by upwelling vapour emanating from the snow a few centimetres under the surface in daytime. Linkletter and Warburton  reported measurements performed at Ross Ice Shelf, which revealed rime and hoar for about 10% of days in the period October-March.
Due to high frequency of hoar formation in the Antarctic plateau, laboratory and field experiments should be performed to study the scavenging process during the formation of crystals on the snow surface. In addition, surface “hoar” crystals should be sampled carefully, by also performing an optical observation to verify if the crystals are unrimed or rimed, i.e. whether they contain spherical microdroplets and microcrystals arising from the freezing of fog droplets. To further highlight the need to take the physics of hydrometeor formation into account to explain snow nitrate concentration, we recall the paper by Wolff et al.  who observed nitrate concentration spikes from day to day in surface snow at Halley (Antarctica), and stated that they could depend on scavenging of fluctuating nitrate concentrations in cloud.
The importance of the physics of precipitation formation processes in determining the chemical composition of the polar snowpack is a general issue, not confined to nitrate. Several papers report a large decrease of within the top metre in low accumulation areas, such as Dome C or Vostok on the East Antarctic Plateau  -  . Lower temperature and higher nss- should reduce loss despite lower accumulation rates  . On the other hand, high accumulation sites (e.g. Summit, Greenland) currently preserve more than 90% of the initial  . Generally speaking, the relationship between accumulation rate and nitrate concentration is complex as the connection between temperature, elevation, accumulation rate and snow pH at the time of deposition makes it difficult to distinguish between the separate effects  .
In order to enhance our understanding of the sources of nitrate found in the ice core and try to reconstruct past atmospheric composition, the nitrogen isotope composition [δ15N] of is considered. The parameter is defined as,
R is the elemental isotope ratio 15N/14N in sample and standard, respectively. Atmospheric nitrogen (N2) has been established as the international reference for 15N/14N.
In the ice core, [δ15N] depends on NOx sources and post-depositional process. Lack of available data on the [δ15N] of NOx sources (lightning, biomass burning, biogenic processes in soils, fossil fuel combustions, oxidation of ammonia) is a limiting factor  . The physical release of HNO3 and photolysis in the UV range has been proposed to explain nitrate loss from snow. The relative importance of the photochemical and physical loss processes at a given site is a key issue to improve the interpretation of the nitrate ice core and determine the nitrate transfer function at the air-snow interface. This requires a knowledge of the nitrogen isotopic fractionation constant associated with each loss process  .
Photolytic fractionation of nitrate in natural snow was studied in a series of experiments by Berhanu et al.  and resulted in significant nitrogen isotopic fractionation that is strongly dependent on the wavelength spectrum of irradiation. At Dome C, photolysis should dominate nitrate loss   . Field studies in the An- tarctic as well as laboratory experiments have shown that the photochemical reduction of nitrates takes place in the superficial liquid-like layer of snow   . This should explain the lower concentration of in sites with low snow accumulation rates.
The relation between the concentrations of ionic substances in precipitating snow and those of their precursors in the air depends largely on the particular mix of scavenging processes active at the time of snow formation (growing crystals, non-growing crystals, rimed or unrimed crystals, dry or wet riming) and during precipitation falling.
Precipitations in polar areas are prevalently in the solid phase. The pristine small ice crystals derived from homogeneous nucleation of super-cooled droplets or heterogeneous nucleation subsequently grow by water vapour diffusion, impaction and freezing of supercooled droplets (riming) and crystal aggregation. Gases and particles are scavenged during in-cloud processes and hydrometeor falling. In addition to hydrometeors formed in cloud, wet deposition includes further processes, i.e. clear-sky precipitations, formation of surface hoar frost (prevalently during night-time), and surface deposition of freezing droplets (rime).
The scavenging efficiency of gases and aerosol differs for each of the above-cited processes. Therefore, even assuming an approximately constant “background” chemical concentration in the atmosphere, the concentration in the deposit should vary with the physics of precipitation formation and the deposition process. This topic is seldom discussed in published papers addressing the relationship between precipitation chemistry and atmospheric chemical composition of gases and aerosols in remote regions.
After carbon dioxide and methane, nitrate (the final product of the oxidation of nitrogen oxides) is the main chemical compound on which researches focus to try to reconstruct past levels of atmospheric nitrogen dioxide from the ice core. In addition to the scavenging processes in the atmosphere, attention must be paid to post-depositional processes which alter nitrate concentration and isotopic composition in deposited snow. The diffusive growth of crystals is prevalent in polar regions due to the high frequency of hoar formation, clear precipitation events, and low frequency of riming process in cloud.
Therefore, additional laboratory and field experiments are required to study the scavenging process during crystal formation, and samplings in field campaigns should be carefully performed for a separate analysis of snow precipitations, cloudless ice crystal precipitation, hoar formation, and surface riming.