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The current described laser set-ups and tethering strategies are compatible with a wide range of rodent behavioral tests. Indeed, a variety of behavioral tests have been used following, or accompanying, in vivo optogenetic stimulation that include emotive behavioral tasks, behavioral conditioning, learning and memory paradigms, sleep, arousal, and appetitive tasks to name a few (see Nieh et al.6 for a comprehensive review). Optogenetics has changed the way traditional behavioral tests are conducted in that multiple-day studies can now be condensed into a single session in which behavior is compared, within-subjects, during distinct epochs of light ‘on’ versus ‘off’5. Of note, behavioral apparatuses that contain doorways, closed compartments or other obstructions may have to be modified to accommodate passage of tethered fibers.
The described tethering strategies permit simultaneous stimulation of multiple mice from a single laser. High throughput optogenetic behavioral testing can therefore be achieved through the use of multiple lasers and testing equipment. The number of animals that can be simultaneously stimulated, however, will be limited by the maximum light power that can be achieved at each fiber tip. Maximum power output at the fiber tip is dependent upon the 1) starting power of the laser; 2) coupling efficiency and 3) number of beam splits. For a 100 mW blue laser with ~80% coupling efficiency and up to 4 beam splits (as depicted in Figure 4C), average power at the fiber tip can range between 5-10 mW when using 200 μm core, 0.22 NA fiber patch cords (n.b. expect transmission loss from rotary joints to be <15%). Measuring light output at the fiber tip is essential for determining adequate light power for opsin activation as opsins differ in their sensitivity to light and therefore the light power density (mW/mm2) required for activation11. For instance, the stable step-function opsin (SSFO) acts as a photon accumulator and therefore requires very little light power density for activation (<8 μW/mm2)8. Compare this to the traditional channel rhodopsin (ChR2) that requires a minimum of 1 mW/mm2 of light to elicit action potentials2. Table 1 is provided as a quick reference for known minimum light irradiances required to activate the most common opsins currently in use. Lastly, one must consider that light scatters and absorbs as it travels through brain tissue such that more light power is required for deeper brain structures3. A useful online resource is available at http://www.stanford.edu/group/dlab/cgi-bin/graph/chart.php that will calculate the light intensity at various depths through brain tissue by taking into account the fiber core size, numerical aperture, wavelength of light used, and the starting light power at the fiber tip. For an excellent overview of the theoretical principles underlying these calculations, see Foutz et al. (2012)12. Examples of how to apply these principles and calculations to experimental design are demonstrated in Aravanis et al. (2007)3 and Tye et al. (2012)13. Performing these calculations prior to the start of an experiment is crucial to ensure adequate light irradiance for opsin activation. Given these considerations, it is advantageous to purchase higher-powered lasers to ensure adequate power output. Lasers with a power output between 100-200 mW are generally sufficient to compensate for small core fibers, multiple fiber splitting, coupling inefficiency and transmission loses7. If using high power lasers, however, care must be taken to avoid neural damage or heat and light-associated artifacts that can occur with prolonged and/or high powered light illumination7. A safe range for in vivo experiments is up to 75 mW/mm2.14
Deciding on the type of laser to purchase can be a complicated matter as there are many factors to consider. For instance, direct diode lasers provide more stable and repeatable pulsed output than do diode-pumped solid-state (DPSS) lasers, and are more reliable over time in a lab environment. In some cases, however, direct diode lasers may emit a lower light power, ~0.1 mW, even when the command voltage is 0 V due to a constant bias current being sent to the diode by the laser’s control electronics. This ‘spontaneous’ emission has a broader spectrum than does laser emission from the same laser, so can be specifically reduced by installing a narrow band-pass (or ‘cleanup’) filter between the laser and coupler (see parts list). This filter will also reduce power output by ~50% when lasing, so purchase a higher-powered laser accordingly. It should be noted that yellow DPSS lasers are extremely sensitive and may behave erratically and have reduced lifespan if rapidly modulated by a pulse generator. Adjustment of yellow laser power should be done through external density filter wheels placed in the beam path (Section 1.7) while operating the laser in TTL+ mode. Alternatively, purchasing a green 532 nm DPSS laser is a cost-effective alternative that can activate both halorhodopsins and archaerhodopsins.
The numerical aperture (NA) of a fiber is important to consider when designing and purchasing fiber components for laser assembly set-up. The NA of an optical fiber determines the angles of light rays that can be accepted and emitted at the tip of a fiber. If a higher-NA fiber is mated to a lower-NA fiber, significant loss will occur at that interface, so it is important to be consistent with fiber NA within a single setup (or to ensure that NA increases along the light path). The effect of fiber NA on the volume of brain tissue illuminated is less important, since brain tissue is highly scattering, and since the light coupled from a laser source will tend to ‘underfill’ high-NA fibers; however optical fibers with an NA of 0.22 and 0.37 are commonly used. Similarly, coupling from a larger-core to a smaller-core fiber will also result in significant losses, so always be sure to use increasing or equal core diameters when progressing from the laser source to the animal implant. On a general note, fiber ends should always be capped when not in use to prevent dust and particulate build-up. It is a good idea to regularly clean fiber ends and connectors (70% isopropyl alcohol works well) to ensure maximal light power output, and to test light power output through a ‘dummy implant’ before beginning each day’s experiments.
During behavioral testing, it is imperative that steps be taken to control for the effects of viral infection, exogenous protein expression, visible light, and possible tissue heating effects and artifacts on animal behavior. Therefore, the proper control group should consist of animals transduced with a control virus (e.g., GFP, eYFP, mCherry) that receive identical light stimulation parameters. Experimental verification is a crucial final step as the behavioral data used for analysis is entirely dependent on proper opsin and fiber optic placement in the region of interest. Specifically, in animals where no immunohistochemical signal is detected, or where placement of signal or fiber is not in the region of interest, then behavioral data for that animal should be removed from the experiment. Additionally, it is essential to test light output at the fiber tip both before surgical implantation and again post-mortem to ensure adequate light power for opsin activation. In animals where severe light loss has occurred through the fiber after experimentation (>30%)9, data for that animal should be considered for removal. Criteria for removal should be established a priori. Finally, one must consider the pulse frequency required to modulate neural firing, which will depend on the brain structure and neuronal sub-types being targeted. Published optogenetic light stimulation parameters exist for multiple neuronal sub-types, however, the ability to modulate neural firing should be independently confirmed through in vivo or brain slice electrophysiological recordings.
As one becomes adept with laser use and modification of laser set-ups, combinations of different wavelengths can be tethered to multiple fibers on a single animal or delivered down the same fiber for combinatorial optogenetics8. Multi-wavelength stimulation will become increasingly important given the rapid development of red-shifted channelrhodopsins8, the engineering of blue-shifted hyperpolarizing opsins15, the use of bistable step-function opsins8,16,17, and the general expanding list of opsins with distinct activation spectra11. This expansion of the optogenetic toolbox will permit the unprecedented control of multiple neural sub-types both within and across brain regions to determine their role in governing complex behavioral states.