Fast Imaging Solar Spectrograph


FISS Summary can be obtained here.

Development of Fast Imaging Solar Spectrograph (FISS) is a collaborative work between Seoul National University (SNU) and Korean Astronomy and Space Science Institute (KASI).

I. Introduction
There exist various kinds of fine structures in the solar chromospheres, like filaments/prominences, jets, spicules, etc. They not only have fine structures, but they also manifest highly dynamic features. Due to limited instrumental resolution up to now, even though these objects have been observed for a long time, it has been difficult to obtain physical properties (temperature, optical thickness, velocities, oscillation frequencies and so on) of these structures with reliability. Identifying physical properties of these fine structures is very essential to understand formation mechanism of the chromospheric features.

    To be fully aware of physical parameters and dynamical features of fine structures, observing instruments should have both high spatial resolution and high spectral resolution, and even high temporal resolution. If New Solar Telescope (NST) of Big Bear Solar Observatory (BBSO) is equipped with FISS which has high spectral resolution, we expect to fulfill required resolution for identifying fine structures.

II. Instrument

Figure 1. Layout of FISS

    FISS is an imaging spectrograph which adopts Echelle disperser with field-scanning method. Single paraboloid mirror is used as both collimator and imager, which can be regarded as quasi-Littrow configuration. Dispersed beams are collected by two CCD cameras that will be preceded by order-selecting narrowband filters, so that images of dual spectral bands can be acquired simultaneously. According to the orientation of the grating, we can get various kinds of dual-band combination. With this dual-band feature, we can distinguish thermal and non-thermal contribution to the spectral line profiles. Some key specifications of FISS are described here below.

 

Item Specification
Lines of interest Ca II (H, K, 8542), Hα, He I 10830Å and so on
Spectral resolving power (Δλ/λ) 1.4 × 105
Field of view 40'' × 60''
Best cadence 10 seconds
Incident F ratio 26
Slit width 16μm
CCD pixels / size 512 × 512 / 16μm × 16μm

Table 1. Specifications of FISS

    FISS is adopting new type of field scanner which consists of two flat mirrors. This design does not require for the scanner to be located at pupil, and it is more compact than K mirror. Linear movement of the scanner makes shift of incident field on slit with preservation of path length.

Figure 2. Concept of two-mirrored field scanner. Thick lines indicate positions of mirrors. Solid black lines and grey dashed line indicate different positions of field scanner.

    According to our simulation, the specifications of FISS were sufficient to identify thread structures in filaments/prominences (Ahn et al., JKAS 2008).

III. Current status and future plan
    As of now, FISS is undergoing lab tests at KASI. Alignment test on a horizontal optical table was successful. The FWHM at the focal plane was 2.5 pixels and this can be regarded as moderate sampling. Still imaging test using coelostat is ongoing. Finally, it should undergo the same procedure on a vertical optical table, which is the same environment at the Coudé lab of NST. Software control for slit scanner and data acquisition from CCD cameras are completed and additional motion controls for mechanical components as grating and CCD cameras are ongoing. We expect the completion of FISS in summer of 2009. And as long as the beam from NST is fed down to Coudé room, we may start the first observation.

Figure 3. Alignment test on a horizontal optical table and imaginary ray path (red arrows)

 

 


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