Page 47 - IJB-3-1
P. 47

Lothar  Koch,  Ole  Brandt,  Andrea  Deiwick,  et  al.

            bubble expands by vapor pressure and propels the ad-
            jacent biomaterial forward, which then is deposited as
            a droplet at a predefined position on a collector slide.













            Figure  1.  Schematic  sketch  of  the  laser-assisted  bioprinting
            technique. The donor slide is coated with a thin laser-absorbing
            layer and a thicker layer of biomaterial to be transferred, usu-
            ally a hydrogel with embedded cells. Laser pulses are focused   Figure 2.  Chart of the laser  wavelengths and pulse durations
            through  the  donor  glass  slide  into  the  absorbing  layer.  The   applied for laser-assisted bioprinting by different groups. Num-
            evaporation of this layer in the laser-focused region generates a   bers in brackets refer to references. Typically, ultraviolet lasers
            high  vapor  pressure  that  propels  the  biomaterial  underneath   and  also  some  infrared  lasers  are  used,  but  not  lasers  in  the
            towards the collector slide.                       visible range (ca. 380–780 nm, colored background). Most com-
                                                               mon are pulse durations in the nanosecond range, but also ex-
               As  a  variant,  some  groups  apply  laser  printing   periments  with  femtosecond  lasers  have  been  conducted.  Na-
            without  dynamic-release  layer.  Therefore,  they  use   nosecond lasers are usually preferred for their compactness and
                                                               relatively simple maintenance and low costs.
            hydrogel (with embedded cells) as the laser-absorbing
            material; a small part of it is vaporized thereby. Some-  Duocastella  et  al. [11]   printed  a  glycerol-water  blend
            times,  they  mix  the  hydrogel  with  a  laser-absorbing   using laser with 1027-nm wavelength and 450-fs pulse
            material, a matrix material with a high absorption co-  duration.  Desrus  et  al. [12]   printed  cell  medium  and  a
            efficient at the applied laser wavelength, which there-  glycerol-water  blend,  as  well  as  keratinocytes  with
            by  will  also  become  part  of  the  printed  structure.   cell  medium  using  1030-nm  laser  wavelength,  and
            However,  DRLs  are  assumed  to  enable  a  printing   350-fs  and  800-fs  pulse  durations.  Due  to  the  high
            more softly and gently for the cells with a higher cell   electro-magnetic  forces  in  the  laser  focus,  these  ul-
            vitality after printing.                           tra-short  pulse  lasers  are  able  to  induce  laser-
               Several  groups  in  the  world  have  developed  self-   absorbing  plasma  in  water  or  hydrogels.  Therefore,
            constructed  laser  bioprinting  setups  with  different   with laser pulse energy high enough, applying a DRL
            pulsed laser systems. Laser parameters vary in a wide   is not necessary [12] .
            range of wavelengths, pulse durations, pulse energies,   In spite of this wide range of applied laser parame-
            and  focal  spot  sizes.  For  the  printing  process,  lasers   ters,  so  far,  their  impact  on  the  transfer  process  has
            with different wavelengths from 193 to 1064 nanome-  hardly  been  analyzed  in  direct  comparison–with  the
            ters and different laser pulse durations, mainly in the   exception of laser pulse energy, laser pulse intensity,
            nanosecond  range,  are  applied  (Figure  2).  They  are   and  the  focal  spot  size.  There  is  one  publication,  in
                                                                              [4]
            combined  with  different  DRL  materials,  including   which Dinca et al.  utilized laser-printed proteins and
            metals (gold, silver, or titanium), polymers (triazene,   DNA  with  500  femtoseconds  of  pulse  duration  at
            polyethylene  naphthalate,  polyimide,  or  cyanoacry-  248-nm  wavelength  and  compared  the  results  with
            late), or hydrogels (gelatin). Most groups using LaBP   those achieved with 15-ns pulse duration.
            for printing biomaterials apply ultraviolet (UV) lasers   To narrow this knowledge gap, we studied the de-
            with  3  to  30  nanoseconds  pulse  durations  and  193-   pendences of printed droplet volume and cell survival
                                              [6]
                                    [5]
            nm [1,2] ,  248-nm [3,4] ,  266-nm ,  337-nm ,  or  355-nm   rate on laser wavelength, pulse duration, pulse power,
            [7,8]  wavelengths.                                and laser intensity in the focal spot. We applied two
               Alternatively, near-infrared (NIR) lasers with 10 or   different  lasers,  a  Nd:YAG  laser  with  three  different
            30  nanoseconds  of  pulse  duration  and  1064-nm [9,10]    wavelengths (1064 nm, 532 nm,  and 355 nm) and a
            wavelength are used in combination with metal DRLs   Yb:YAG laser with the pulse durations in the range of
            (usually gold). Also femtosecond lasers were applied.     8 to 200 nanoseconds at 1064-nm wavelength.

                                        International Journal of Bioprinting (2017)–Volume 3, Issue 1      43
   42   43   44   45   46   47   48   49   50   51   52