You have requested a machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Neither SPIE nor the owners and publishers of the content make, and they explicitly disclaim, any express or implied representations or warranties of any kind, including, without limitation, representations and warranties as to the functionality of the translation feature or the accuracy or completeness of the translations.
Translations are not retained in our system. Your use of this feature and the translations is subject to all use restrictions contained in the Terms and Conditions of Use of the SPIE website.
The concept of photonic and phononic crystal sensors is based on the measurement of changes in the transmission
properties of the devices caused by changes of material properties of one of the materials building the crystal. It has been
demonstrated that in the optical case the key parameter is the refractive index, i.e. speed of light, in the acoustic case it is
sound velocity. Both parameters can be measured with accuracy competitive with other optical and acoustic sensor
principles. A phoxonic crystal sensor combines both concepts in one device, therefore allowing for a dual parallel
determination of two independent material properties. Such a sensor is especially attractive for complex analytes as
common in chemistry and biochemistry. We have designed and modeled a phoxonic crystal consisting of a solid matrix
and holes where the central cavity acts as analyte container. We especially concentrate on the generation of a
characteristic feature within the transmission spectrum like a transmission peak within the phoxonic band gap where the
respective wavelength or frequency of maximum transmission is sensitive to material properties of the analyte. We could
show theoretically that a (geometric) defect is required in photonics whereas in phononics separation of the sensitive
peak is the challenge. The respective wavelength/frequency of maximum transmission moves in accordance to the
resonance conditions. We further analyze the transmission of light and sound through a phoxonic crystal plate at normal incidence.