CN108917923B - Power measurement method and electronic equipment - Google Patents
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Abstract
本发明公开了一种功率测量方法和电子设备,涉及光学领域,应用于电子设备,该电子设备包括:滤波单元、功率测量单元和多个光谱测量单元,该方法包括:通过多个该光谱测量单元,对来自超连续谱光源的光束进行测量,得到该光束的多个波段的光谱数据。将该多个波段的光谱数据进行拼接,得到该光束的总光谱数据。通过该滤波单元,对来自该超连续谱光源的光束进行滤波处理,得到预设波段的光束。通过该功率测量单元,对该预设波段的光束进行测量,得到该预设波段的光束的功率。根据该光束的总光谱数据和该预设波段的光束的功率,生成该光束的总功率。该方法可提高测量超连续谱光源的总功率的精确度。
The invention discloses a power measurement method and electronic equipment, which relate to the field of optics and are applied to electronic equipment. The electronic equipment includes: a filter unit, a power measurement unit, and a plurality of spectrum measurement units. The method includes: measuring The unit measures the light beam from the supercontinuum light source, and obtains the spectral data of multiple bands of the light beam. The spectral data of the multiple bands are spliced to obtain the total spectral data of the beam. Through the filtering unit, the light beam from the supercontinuum light source is filtered to obtain the light beam of the preset wavelength band. The power measurement unit measures the light beam of the preset waveband to obtain the power of the light beam of the preset waveband. The total power of the beam is generated according to the total spectral data of the beam and the power of the beam in the preset wavelength band. The method can improve the accuracy of measuring the total power of a supercontinuum light source.
Description
技术领域technical field
本发明涉及光学领域,尤其涉及一种功率测量方法和电子设备。The invention relates to the field of optics, in particular to a power measurement method and electronic equipment.
背景技术Background technique
随着近年来科学技术的快速发展,超连续谱光源以其高亮度、高相干性和超带宽等优点广泛应用于光谱学、环境监测、化学传感、生物化学以及红外线对抗等民用和军事领域。目前通常采用激光功率计测量超连续谱光源的总功率,但是超连续光谱光源的带宽极宽,激光功率计的测量范围有限,因此需采取多个激光功率计对超连续谱光源进行测量,而不同的激光功率计对于不同波段的激光功率的标定方法不同,因此存在超连续谱光源的总功率的测量不够精确的问题。With the rapid development of science and technology in recent years, supercontinuum light sources are widely used in civil and military fields such as spectroscopy, environmental monitoring, chemical sensing, biochemistry, and infrared countermeasures due to their high brightness, high coherence, and ultra-bandwidth. . At present, laser power meters are usually used to measure the total power of supercontinuum light sources, but the bandwidth of supercontinuum light sources is extremely wide, and the measurement range of laser power meters is limited. Therefore, multiple laser power meters are required to measure supercontinuum light sources. Different laser power meters have different calibration methods for laser power in different bands, so there is a problem that the measurement of the total power of the supercontinuum light source is not accurate enough.
发明内容Contents of the invention
本发明实施例的主要目的在于提供一种功率测量方法和电子设备,可提高测量超连续谱光源的总功率的精确度。The main purpose of the embodiments of the present invention is to provide a power measurement method and electronic equipment, which can improve the accuracy of measuring the total power of a supercontinuum light source.
本发明实施例第一方面提供了一种功率测量方法,应用于电子设备,所述电子设备包括:滤波单元、功率测量单元和多个光谱测量单元,所述方法包括:通过多个所述光谱测量单元,对来自超连续谱光源的光束进行测量,得到所述光束的多个波段的光谱数据;将所述多个波段的光谱数据进行拼接,得到所述光束的总光谱数据;通过所述滤波单元,对来自所述超连续谱光源的光束进行滤波处理,得到预设波段的光束;通过所述功率测量单元,对所述预设波段的光束进行测量,得到所述预设波段的光束的功率;根据所述光束的总光谱数据和所述预设波段的光束的功率,生成所述光束的总功率。The first aspect of the embodiments of the present invention provides a power measurement method, which is applied to electronic equipment, and the electronic equipment includes: a filter unit, a power measurement unit, and a plurality of spectrum measurement units, and the method includes: using a plurality of the spectrum The measuring unit measures the light beam from the supercontinuum light source to obtain spectral data of multiple bands of the light beam; splicing the spectral data of the multiple bands to obtain the total spectral data of the light beam; through the A filtering unit is configured to filter the beam from the supercontinuum light source to obtain a beam of a preset band; through the power measurement unit, measure the beam of the preset band to obtain a beam of the preset band the power of the light beam; generating the total power of the light beam according to the total spectral data of the light beam and the power of the light beam in the preset wavelength band.
本发明实施例第二方面提供了一种电子设备,所述电子设备包括:多个光谱测量单元,用于对来自超连续谱光源的光束进行测量,得到所述光束的多个波段的光谱数据;拼接单元,与多个所述光谱测量单元相连,用于将所述多个波段的光谱数据进行拼接,得到所述光束的总光谱数据;滤波单元,用于对来自所述超连续谱光源的光束进行滤波处理,得到预设波段的光束;功率测量单元,与所述滤波单元相连,用于对所述预设波段的光束进行测量,得到所述预设波段的光束的功率;生成单元,与所述拼接单元和所述功率测量单元相连,用于根据所述光束的总光谱数据和所述预设波段的光束的功率,生成所述光束的总功率。The second aspect of the embodiment of the present invention provides an electronic device, the electronic device includes: a plurality of spectral measurement units, used to measure the light beam from the supercontinuum light source, and obtain the spectral data of multiple bands of the light beam The splicing unit is connected to a plurality of the spectral measurement units, and is used to splice the spectral data of the multiple bands to obtain the total spectral data of the light beam; the filtering unit is used to filter the light from the supercontinuum The light beam is filtered to obtain the light beam of the preset waveband; the power measurement unit is connected to the filtering unit, and is used to measure the light beam of the preset waveband to obtain the power of the light beam of the preset waveband; the generation unit , connected to the splicing unit and the power measuring unit, configured to generate the total power of the light beam according to the total spectral data of the light beam and the power of the light beam in the preset wavelength band.
从上述实施例可知,通过多个光谱测量单元直接测量得到多个波段的光谱数据,通过滤波单元对光源进行滤波得到预设波段的光束,并通过功率测量单元直接测量该预设波段的光束,然后通过直接测量得到的多个波段的光谱数据和预设波段的功率计算得到光源的总功率,而不需利用不同波段的功率计对光源进行测量并求和得到光源的总功率,从而避免了不同波段的功率计的标定方法不同所引起的误差,进而提高了测量超连续谱光源的总功率的精确度。It can be seen from the above-mentioned embodiments that the spectral data of multiple bands is obtained by direct measurement through multiple spectral measurement units, the light source is filtered by the filter unit to obtain the beam of the preset band, and the beam of the preset band is directly measured by the power measurement unit, Then calculate the total power of the light source by directly measuring the spectral data of multiple bands and the power of the preset bands, without using power meters in different bands to measure the light source and sum to obtain the total power of the light source, thus avoiding the The errors caused by different calibration methods of power meters in different bands further improve the accuracy of measuring the total power of supercontinuum light sources.
附图说明Description of drawings
图1是本发明提供的第一实施例中的功率测量方法的应用示意图;FIG. 1 is a schematic diagram of the application of the power measurement method in the first embodiment provided by the present invention;
图2是本发明提供的第一实施例中的功率测量方法的实现流程示意图;Fig. 2 is a schematic diagram of the implementation flow of the power measurement method in the first embodiment provided by the present invention;
图3是本发明提供的第二实施例中的功率测量方法的实现流程示意图;Fig. 3 is a schematic diagram of the implementation flow of the power measurement method in the second embodiment provided by the present invention;
图4是本发明提供的第三实施例中的电子设备的结构示意图。Fig. 4 is a schematic structural diagram of an electronic device in a third embodiment provided by the present invention.
具体实施方式Detailed ways
为使得本发明的发明目的、特征、优点能够更加的明显和易懂,下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅仅是本发明一部分实施例,而非全部实施例。基于本发明中的实施例,本领域技术人员在没有做出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。In order to make the purpose, features and advantages of the present invention more obvious and understandable, the technical solutions in the embodiments of the present invention will be clearly and completely described below in conjunction with the accompanying drawings in the embodiments of the present invention. Obviously, the described The embodiments are only some of the embodiments of the present invention, but not all of them. Based on the embodiments of the present invention, all other embodiments obtained by those skilled in the art without making creative efforts belong to the protection scope of the present invention.
参见图1,图1是本发明提供的第一实施例中的功率测量方法的应用示意图,该方法应用于电子设备。如图1所示,该电子设备包括滤波单元101、功率测量单元102和多个光谱测量单元103。示例性的,多个光谱测量单元103通过多模光纤跳线104接收来自超连续谱光源105的光束进行测量。滤波单元101可为带通滤波器,功率测量单元102可为激光功率计,光谱测量单元103可为光谱仪。Referring to FIG. 1 , FIG. 1 is a schematic diagram of the application of the power measurement method in the first embodiment provided by the present invention, and the method is applied to electronic equipment. As shown in FIG. 1 , the electronic device includes a
参见图2,图2是本发明提供的第一实施例中的功率测量方法的实现流程示意图。如图2所示,该功率测量方法包括:Referring to FIG. 2 , FIG. 2 is a schematic flowchart of an implementation of the power measurement method in the first embodiment provided by the present invention. As shown in Figure 2, the power measurement method includes:
201、通过多个光谱测量单元,对来自超连续谱光源的光束进行测量,得到该光束的多个波段的光谱数据。201. Using multiple spectral measurement units, measure the light beam from the supercontinuum light source to obtain spectral data of multiple bands of the light beam.
具体的,由于超连续谱光源具有带宽极宽的特点,而单个光谱测量单元的测量范围有限,因此采用多个不同测量范围的光谱测量单元,对来自超连续谱光源的光束进行测量,相应的,各光谱测量单元测量该光束后得到位于自身测量范围内的光谱数据。也就是说,各光谱测量单元测量得到的光谱数据的波段不大于各光谱测量单元的测量范围。可以理解的,为了获取超连续谱光源的全带宽的光谱数据,因此多个光谱测量单元的测量范围的和包括超连续谱光源的全带宽。Specifically, since the supercontinuum light source has the characteristics of extremely wide bandwidth, and the measurement range of a single spectral measurement unit is limited, multiple spectral measurement units with different measurement ranges are used to measure the beam from the supercontinuum light source, and the corresponding , each spectral measurement unit measures the light beam to obtain spectral data within its own measurement range. That is to say, the wavelength band of the spectral data measured by each spectral measurement unit is not larger than the measurement range of each spectral measurement unit. It can be understood that, in order to obtain spectral data of the full bandwidth of the supercontinuum light source, the sum of the measurement ranges of the multiple spectral measurement units includes the full bandwidth of the supercontinuum light source.
202、将该多个波段的光谱数据进行拼接,得到该光束的总光谱数据。202. Splice the spectral data of the multiple bands to obtain the total spectral data of the light beam.
具体的,由于各光谱测量单元测量得到的光谱数据是来自超连续谱光源的光束的部分波段的光谱数据,因此,将各光谱测量单元测量得到的多个光谱数据进行拼接,而多个光谱数据所对应的波段不相同,也就是说,将各个波段的光谱数据进行拼接,以得到该光束的总光谱数据。Specifically, since the spectral data measured by each spectral measurement unit is the spectral data of a partial band of the light beam from the supercontinuum light source, the multiple spectral data measured by each spectral measurement unit are spliced, and the multiple spectral data The corresponding wavebands are different, that is to say, the spectral data of each waveband are spliced to obtain the total spectral data of the beam.
203、通过该滤波单元,对来自该超连续谱光源的光束进行滤波处理,得到预设波段的光束。203. Using the filtering unit, perform filtering processing on the light beam from the supercontinuum light source to obtain a light beam in a preset wavelength band.
具体的,由于来自超连续谱光源的光束的带宽极宽,而功率测量单元的测量范围有限,因此,在通过功率测量单元测量之前,通过滤波单元将该光束进行滤波处理,以得到预设波段的光束。在实际应用中,滤波单元可为带通滤波器,带通滤波器是一个允许特定频段的波通过同时屏蔽其他频段的设备,则可以理解的,该滤波单元允许通过的波段为该预设波段的光束的波段,该预设波段的光束的波段位于来自超连续谱光源的光束的带宽内。Specifically, since the bandwidth of the light beam from the supercontinuum light source is extremely wide, and the measurement range of the power measurement unit is limited, the light beam is filtered by the filtering unit before being measured by the power measurement unit to obtain a preset wavelength band Beam. In practical applications, the filter unit can be a band-pass filter, which is a device that allows waves of a specific frequency band to pass through while shielding other frequency bands. It can be understood that the band that the filter unit allows to pass is the preset band The wavelength band of the beam of the preset wavelength band is within the bandwidth of the beam from the supercontinuum light source.
204、通过该功率测量单元,对该预设波段的光束进行测量,得到该预设波段的光束的功率。204. Use the power measurement unit to measure the light beam in the preset wavelength band to obtain the power of the light beam in the preset wave band.
具体的,通过滤波单元将该光束进行滤波处理后,得到预设波段的光束,接着通过功率测量单元将该预设波段的光束进行测量,以获取该预设波段的光束的功率。可以理解的,该预设波段的光束的波段不大于功率测量单元的测量范围,该功率测量单元的测量范围小于来自超连续谱光源的光束的带宽。Specifically, after the light beam is filtered by the filtering unit, the light beam of the preset waveband is obtained, and then the light beam of the preset waveband is measured by the power measurement unit to obtain the power of the light beam of the preset waveband. It can be understood that the wavelength band of the light beam of the preset wavelength band is not larger than the measurement range of the power measurement unit, and the measurement range of the power measurement unit is smaller than the bandwidth of the light beam from the supercontinuum light source.
205、根据该光束的总光谱数据和该预设波段的光束的功率,生成该光束的总功率。205. Generate the total power of the beam according to the total spectral data of the beam and the power of the beam in the preset wavelength band.
具体的,通过将多个波段的光谱数据进行拼接得到的总光谱数据,以及通过功率测量单元测量得到的预设波段的光束的功率,生成该光束的总功率。在该过程中,仅需一个功率测量单元即可通过后续计算得到光束的总功率。Specifically, the total power of the light beam is generated by splicing the spectral data of multiple bands to obtain the total spectral data and the power of the light beam of the preset wave band measured by the power measurement unit. In this process, only one power measurement unit is needed to obtain the total power of the beam through subsequent calculation.
在本发明实施例中,通过多个光谱测量单元直接测量得到多个波段的光谱数据,通过滤波单元对光源进行滤波得到预设波段的光束,并通过功率测量单元直接测量该预设波段的光束,然后通过直接测量得到的多个波段的光谱数据和预设波段的功率计算得到光源的总功率,而不需利用不同波段的功率计对光源进行测量并求和得到光源的总功率,从而避免了不同波段的功率计的标定方法不同所引起的误差,进而提高了测量超连续谱光源的总功率的精确度。In the embodiment of the present invention, the spectral data of multiple bands is directly measured by multiple spectral measurement units, the light source is filtered by the filtering unit to obtain the beam of the preset band, and the beam of the preset band is directly measured by the power measurement unit , and then calculate the total power of the light source by directly measuring the spectral data of multiple bands and the power of the preset bands, without using power meters in different bands to measure the light source and sum to obtain the total power of the light source, thereby avoiding The error caused by different calibration methods of power meters in different bands is eliminated, and the accuracy of measuring the total power of supercontinuum light sources is improved.
参见图3,图3是本发明提供的第二实施例中的功率测量方法的实现流程示意图,该功率测量方法应用于电子设备。如图3所示,该方法主要包括以下步骤:Referring to FIG. 3 , FIG. 3 is a schematic flowchart of an implementation of a power measurement method in a second embodiment provided by the present invention, and the power measurement method is applied to an electronic device. As shown in Figure 3, the method mainly includes the following steps:
301、通过多个光谱测量单元,对来自超连续谱光源的光束进行测量,得到该光束的多个波段的光谱数据。301. Measure a light beam from a supercontinuum light source by using multiple spectral measurement units, and obtain spectral data of multiple wavelength bands of the light beam.
302、将该线性光谱数据转换为转换对数光谱数据,并在该对数光谱数据和该转换对数光谱数据中选取任意一个光谱数据作为基准对数光谱数据。302. Convert the linear spectral data into transformed logarithmic spectral data, and select any spectral data from the logarithmic spectral data and the transformed logarithmic spectral data as the reference logarithmic spectral data.
具体的,由于部分光谱测量单元测量光束得到的是对数光谱数据,而部分光谱测量单元测量光束得到的是线性光谱数据,因此该多个波段的光谱数据中若干波段的光谱数据为对数光谱数据,剩余波段的光谱数据为线性光谱数据。为了进一步将多个光谱数据进行处理,将线性光谱数据转换为转换对数光谱数据。可选的,采用如下公式将线性光谱数据转换为转换对数光谱数据:Specifically, because part of the spectral measurement unit measures the light beam to obtain logarithmic spectral data, and part of the spectral measurement unit measures the light beam to obtain linear spectral data, so the spectral data of several bands in the spectral data of multiple bands are logarithmic spectra data, and the spectral data of the remaining bands are linear spectral data. In order to further process multiple spectral data, the linear spectral data is converted into transformed logarithmic spectral data. Optionally, use the following formula to convert linear spectral data into transformed logarithmic spectral data:
y=-10lg(x)y=-10lg(x)
式中,x是光谱测量单元测量所得的某波长的线性强度值,y是对应波长的对数强度值。In the formula, x is the linear intensity value of a certain wavelength measured by the spectral measurement unit, and y is the logarithmic intensity value of the corresponding wavelength.
其中,对数光谱数据和转换对数光谱数据均为波长与对应波长的对数强度值的形式,在对数光谱数据和转换对数光谱数据中,选取任意一个光谱数据作为基准对数光谱数据。Among them, the logarithmic spectral data and transformed logarithmic spectral data are both in the form of wavelength and the logarithmic intensity value of the corresponding wavelength. Among the logarithmic spectral data and transformed logarithmic spectral data, any spectral data is selected as the reference logarithmic spectral data .
可选的,在对数光谱数据和转换对数光谱数据中选取包含有最小波长的光谱数据作为基准光谱数据,或者,在对数光谱数据和转换对数光谱数据中选取包含有来自超连续谱光源的光束的中间波长的光谱数据作为基准数据,或者,在对数光谱数据和转换对数光谱数据中选取包含有最大波长的光谱数据作为基准光谱数据。Optionally, in the logarithmic spectral data and converted logarithmic spectral data, select the spectral data containing the minimum wavelength as the reference spectral data, or, in the logarithmic spectral data and transformed logarithmic spectral data, select the spectral data containing the data from the supercontinuum The spectral data of the intermediate wavelength of the light beam of the light source is used as the reference data, or the spectral data including the maximum wavelength is selected from the logarithmic spectral data and the converted logarithmic spectral data as the reference spectral data.
303、在剩下的该对数光谱数据和该转换对数光谱数据中,选取对应的波段与该基准对数光谱数据的波段有重合的光谱数据,作为待拼接对数光谱数据。303. From the remaining logarithmic spectral data and the converted logarithmic spectral data, select spectral data whose corresponding waveband overlaps with the waveband of the reference logarithmic spectral data, as the logarithmic spectral data to be spliced.
具体的,在除基准对数光谱数据外的对数光谱数据和转换对数光谱数据中,选取与基准对数光谱数据的波段有重合的光谱数据,作为待拼接对数光谱数据。示例性的,基准对数光谱数据的波段为350~750nm(单位:纳米),剩下两个光谱数据的波段分别为:650~1250nm和1150~1700nm,其中,波段范围为650~1250nm的光谱数据与基准光谱数据的波段有重合,波段范围为1150~1700nm的光谱数据与基准光谱数据的波段无重合,因此,波段范围为650~1250nm的光谱数据为待拼接对数光谱数据。Specifically, among the logarithmic spectral data and converted logarithmic spectral data except the reference logarithmic spectral data, the spectral data overlapping with the band of the reference logarithmic spectral data is selected as the logarithmic spectral data to be spliced. Exemplarily, the waveband of the reference logarithmic spectral data is 350-750nm (unit: nanometer), and the wavebands of the remaining two spectral data are: 650-1250nm and 1150-1700nm, wherein the waveband range is the spectrum of 650-1250nm The bands of the data overlap with the reference spectral data, and the spectral data with a band range of 1150-1700nm does not overlap with the reference spectral data. Therefore, the spectral data with a band range of 650-1250nm is the logarithmic spectral data to be spliced.
304、基于该基准对数光谱数据和该待拼接对数光谱数据的重合波段,按照预设算法计算得到连接波长。304. Based on the overlapping bands of the reference logarithmic spectral data and the logarithmic spectral data to be spliced, calculate and obtain the connection wavelength according to a preset algorithm.
具体的,由于光谱测量单元的测量范围的边界导致的误差和不确定性增大,因此在确定基准对数光谱数据和待拼接光谱数据的重合波段后,不选取重合波段的边界的波长作为连接波长,而是按照预设算法根据重合波段计算得到连接波长,该预设算法可根据实际情况进行设计。示例性的,基准对数光谱数据的波段为350~750nm,待拼接对数光谱数据的波段范围为650~1250nm,基准对数光谱数据和待拼接对数光谱数据的重合波段为650~750nm,则可选取该重合波段的中间波长作为连接波长,也就是说,按照(650+750)÷2=700nm计算得到700nm作为连接波长。Specifically, due to the increased error and uncertainty caused by the boundary of the measurement range of the spectral measurement unit, after determining the overlapping bands of the reference logarithmic spectral data and the spectral data to be spliced, the wavelength of the boundary of the overlapping bands is not selected as the connection Instead, the connection wavelength is calculated according to the overlapping bands according to a preset algorithm, which can be designed according to the actual situation. Exemplarily, the wavelength band of the reference logarithmic spectral data is 350-750nm, the wavelength range of the logarithmic spectral data to be spliced is 650-1250nm, and the overlapping band of the reference logarithmic spectral data and the logarithmic spectral data to be spliced is 650-750nm, Then, the middle wavelength of the overlapped band can be selected as the connection wavelength, that is, 700 nm is obtained as the connection wavelength calculated according to (650+750)÷2=700 nm.
305、在该基准对数光谱数据和该待拼接对数光谱数据中,分别获取与该连接波长相应的基准对数强度值和待拼接对数强度值;305. From the reference logarithmic spectral data and the logarithmic spectral data to be spliced, respectively obtain a reference logarithmic intensity value and a logarithmic intensity value to be spliced corresponding to the connection wavelength;
306、将该待拼接对数强度值减去该基准对数强度值,得到偏差值,并根据该偏差值,将该待拼接对数光谱数据中的全部对数强度值减去该偏差值,以将该待拼接对数光谱数据和该基准对数光谱数据在该连接波长处拼接在一起,将拼接后的该基准对数光谱数据和该待拼接对数光谱数据作为新的基准对数光谱数据。306. Subtracting the reference logarithmic intensity value from the logarithmic intensity value to be spliced to obtain a deviation value, and subtracting the deviation value from all logarithmic intensity values in the logarithmic spectrum data to be spliced according to the deviation value, The logarithmic spectral data to be spliced and the reference logarithmic spectral data are spliced together at the connection wavelength, and the spliced reference logarithmic spectral data and the logarithmic spectral data to be spliced are used as a new reference logarithmic spectrum data.
具体的,理论上而言,对于来自相同光源的光束的某个波长的强度值应为一个定值,但是由于不同的光谱测量单元之间存在的系统误差,对于来自同一个光源的相同波长测量得到的强度值会存在误差,因此获取到的与连接波长对应的基准对数强度值和待拼接对数强度值可能存在不相等的情况。Specifically, in theory, the intensity value of a certain wavelength of the beam from the same light source should be a constant value, but due to the systematic error between different spectral measurement units, for the same wavelength measurement from the same light source There will be errors in the obtained intensity value, so the acquired reference logarithmic intensity value corresponding to the connection wavelength and the logarithmic intensity value to be spliced may not be equal.
因此,将待拼接对数强度值减去基准对数强度值,得到偏差值。可以理解的,该偏差值可为零。确定偏差值后,说明待拼接对数光谱数据的对数强度值整体相当于基准对数强度值的误差为该偏差值,因此,将待拼接对数光谱数据中的全部对数强度值减去该偏差值,以使连接波长处的待拼接对数强度值与连接波长处的基准对数强度值相等,也就是说,基准对数光谱数据的连接波长处的点和待拼接对数光谱数据的连接波长处的点可重合,将该点重合后,可视为在横坐标为波长、纵坐标为对数强度的坐标系中,将基准对数光谱数据和待拼接对数光谱数据拼接在了一起。可以理解的,基准对数光谱数据和待拼接对数光谱数据相并形成了一个新的光谱数据集,该新的光谱数据集为新的基准对数光谱数据。Therefore, subtract the reference logarithmic intensity value from the logarithmic intensity value to be spliced to obtain the deviation value. Understandably, the deviation value may be zero. After determining the deviation value, it means that the error of the logarithmic intensity value of the logarithmic spectral data to be spliced is equivalent to the reference logarithmic intensity value as the deviation value. Therefore, subtract all logarithmic intensity values in the logarithmic spectral data to be spliced The deviation value is to make the logarithmic intensity value to be spliced at the connecting wavelength equal to the reference logarithmic intensity value at the connecting wavelength, that is, the point at the connecting wavelength of the reference logarithmic spectral data and the logarithmic spectral data to be spliced The points at the connecting wavelengths can be coincident. After the points coincide, it can be regarded as splicing the reference logarithmic spectral data and the logarithmic spectral data to be spliced in the coordinate system where the abscissa is the wavelength and the ordinate is the logarithmic intensity. together. It can be understood that the reference logarithmic spectral data and the logarithmic spectral data to be spliced are combined to form a new spectral data set, and the new spectral data set is the new reference logarithmic spectral data.
其中,基于该新的基准对数光谱数据,重复执行步骤303-306,当没有剩下的对数光谱数据和转换对数光谱数据时,执行步骤307:直至将该多个波段的光谱数据全部拼接在一起,得到该光束的总对数光谱数据。Wherein, based on the new reference logarithmic spectral data, steps 303-306 are repeatedly executed, and when there is no remaining logarithmic spectral data and transformed logarithmic spectral data,
308、将该光束的总对数光谱数据进行转换,得到该光束的总线性光谱数据。308. Convert the total logarithmic spectral data of the light beam to obtain the total linear spectral data of the light beam.
具体的,为了便于后续计算该光束的总功率,将该光束的总对数光谱数据进行转换,得到该光束的总线性光谱数据。示例性的,可按照如下公式进行转换:Specifically, in order to facilitate subsequent calculation of the total power of the beam, the total logarithmic spectrum data of the beam is converted to obtain the total linear spectrum data of the beam. Exemplarily, conversion can be performed according to the following formula:
式中,x是总对数光谱数据中的某波长对应的对数强度值,y是对应波长的线性强度值。In the formula, x is the logarithmic intensity value corresponding to a certain wavelength in the total logarithmic spectral data, and y is the linear intensity value corresponding to the wavelength.
309、通过该滤波单元,对来自该超连续谱光源的光束进行滤波处理,得到预设波段的光束。309. Through the filtering unit, filter the light beam from the supercontinuum light source to obtain a light beam in a preset wavelength band.
310、通过该功率测量单元,对该预设波段的光束进行测量,得到该预设波段的光束的功率。310. Using the power measurement unit, measure the light beam in the preset wavelength band to obtain the power of the light beam in the preset wave band.
311、将该光束的总线性光谱数据进行求和,得到该光束的光谱总强度;在该光束的总线性光谱数据中选取该预设波段的光谱数据并进行求和,得到该预设波段的光束的光谱强度;根据该光束的光谱总强度、该预设波段的光束的光谱强度和该预设波段的光束的功率,生成该光束的总功率。311. Sum the total linear spectral data of the light beam to obtain the total spectral intensity of the light beam; select and sum the spectral data of the preset band from the total linear spectral data of the light beam to obtain the spectral data of the preset band The spectral intensity of the light beam; according to the total spectral intensity of the light beam, the spectral intensity of the light beam in the preset wavelength band and the power of the light beam in the preset wave band, the total power of the light beam is generated.
具体的,将该光束的总线性光谱数据进行求和,即将该光束的总线性光谱强度进行积分,积分的下限为该总线性光谱数据中的最小波长,该积分的上限为该总线性光谱数据中的最大波长,以得到该光束的光谱总强度。Specifically, the total linear spectral data of the light beam is summed, that is, the total linear spectral intensity of the light beam is integrated, the lower limit of the integral is the minimum wavelength in the total linear spectral data, and the upper limit of the integral is the total linear spectral data The maximum wavelength in to get the total spectral intensity of the beam.
因为预设波段被包含在总线性光谱数据的波段中,因此为求得该预设波段的光束的光谱强度,可在该光束的总线型光谱数据中选取该预设波段的光谱数据进行求和,即将该预设波段的光谱数据进行积分,积分的下限为该预设波段的最小波长,积分的上限为该预设波段的最大波长。Because the preset band is included in the band of the total linear spectral data, in order to obtain the spectral intensity of the beam of the preset band, the spectral data of the preset band can be selected from the bus type spectral data of the beam for summation , that is to integrate the spectral data of the preset band, the lower limit of the integration is the minimum wavelength of the preset band, and the upper limit of the integration is the maximum wavelength of the preset band.
其中,可按照如下公式,根据该光束的光谱总强度、该预设波段的光束的光谱强度和该预设波段的光束的功率,生成该光束的总功率:Wherein, according to the following formula, the total power of the beam can be generated according to the total spectral intensity of the beam, the spectral intensity of the beam in the preset band and the power of the beam in the preset band:
式中,P总表示该光束的总功率,S总表示该光束的光谱总强度,S表示该预设波段的光束的光谱强度,P表示该预设波段的光束的功率。In the formula, P always represents the total power of the beam, S always represents the total spectral intensity of the beam, S represents the spectral intensity of the beam in the preset band, and P represents the power of the beam in the preset band.
可选的,将该光束的光谱总强度除以该光束的总功率,得到该光束的光谱总强度和该光束的总功率之间的比例值。Optionally, the total spectral intensity of the light beam is divided by the total power of the light beam to obtain a ratio between the total spectral intensity of the light beam and the total power of the light beam.
将该光束的光谱总强度中的全部的强度值除以该比例值,得到该光束的光谱功率密度数据。All the intensity values in the total spectral intensity of the light beam are divided by the ratio value to obtain the spectral power density data of the light beam.
具体的,功率密度是表征超连续谱光源性能的重要参量,是评判光源质量的重要标准,其单位一般为mw/nm(单位:毫瓦/纳米)。光束的光谱强度分布与光谱功率密度分布之间存在一定的关系,某个波段的光谱强度越大,说明该波段的光谱功率密度越大。因此在得到光束的光谱总强度后。将该光束的光谱总强度除以该光束的总功率,得到该光束的光谱总强度和该光束的总功率之间的比例值。将该线性光谱强度的所有数据都分别除以该斜率,得到该光束的功率密度数据,将该光束的光谱总强度中的全部的强度值除以该比例值,得到该光束的光谱功率密度数据。Specifically, the power density is an important parameter to characterize the performance of a supercontinuum light source and an important criterion for judging the quality of a light source, and its unit is generally mw/nm (unit: milliwatt/nanometer). There is a certain relationship between the spectral intensity distribution of the beam and the spectral power density distribution. The greater the spectral intensity of a certain band, the greater the spectral power density of this band. Therefore, after obtaining the total spectral intensity of the beam. The total spectral intensity of the beam is divided by the total power of the beam to obtain a ratio value between the total spectral intensity of the beam and the total power of the beam. Divide all the data of the linear spectral intensity by the slope to obtain the power density data of the beam, divide all the intensity values in the total spectral intensity of the beam by the ratio value, and obtain the spectral power density data of the beam .
可选的,为了提高光束的总对数光谱数据、总线性光谱数据和光谱功率密度数据的直观性和便利性,根据该光束的总对数光谱数据、该光束的总线性光谱数据和该光束的光谱功率密度数据进行绘制,分别得到该光束的总对数光谱图、该光束的总线性光谱图和该光束的功率密度分布图。Optionally, in order to improve the intuition and convenience of the total logarithmic spectral data, total linear spectral data and spectral power density data of the beam, according to the total logarithmic spectral data of the beam, the total linear spectral data of the beam and the The spectral power density data of the beam is plotted to obtain the total logarithmic spectrum of the beam, the total linear spectrum of the beam and the power density distribution of the beam.
在本发明实施例中,通过多个光谱测量单元直接测量得到多个波段的光谱数据,通过滤波单元对光源进行滤波得到预设波段的光束,并通过功率测量单元直接测量该预设波段的光束,然后通过直接测量得到的多个波段的光谱数据和预设波段的功率计算得到光源的总功率,而不需利用不同波段的功率计对光源进行测量并求和得到光源的总功率,从而避免了不同波段的功率计的标定方法不同所引起的误差,进而提高了测量超连续谱光源的总功率的精确度。并且,通过将总对数光谱数据、总线性光谱数据和光谱功率密度数据进行绘图,提高了本方法的直观性和便利性。In the embodiment of the present invention, the spectral data of multiple bands is directly measured by multiple spectral measurement units, the light source is filtered by the filtering unit to obtain the beam of the preset band, and the beam of the preset band is directly measured by the power measurement unit , and then calculate the total power of the light source by directly measuring the spectral data of multiple bands and the power of the preset bands, without using power meters in different bands to measure the light source and sum to obtain the total power of the light source, thereby avoiding The error caused by different calibration methods of power meters in different bands is eliminated, and the accuracy of measuring the total power of supercontinuum light sources is improved. Moreover, the intuition and convenience of the method are improved by plotting the total logarithmic spectral data, total linear spectral data and spectral power density data.
参见图4,图4是本发明提供的第三实施例中的电子设备的结构示意图。。如图4所示,该电子设备主要包括:Referring to FIG. 4 , FIG. 4 is a schematic structural diagram of an electronic device in a third embodiment provided by the present invention. . As shown in Figure 4, the electronic equipment mainly includes:
多个光谱测量单元401,用于对来自超连续谱光源的光束进行测量,得到光束的多个波段的光谱数据。A plurality of
拼接单元402,与多个光谱测量单元401相连,用于将多个波段的光谱数据进行拼接,得到光束的总光谱数据。The
滤波单元403,用于对来自超连续谱光源的光束进行滤波处理,得到预设波段的光束。The
功率测量单元404,与滤波单元403相连,用于对预设波段的光束进行测量,得到预设波段的光束的功率。The
生成单元405,与拼接单元402和功率测量单元404相连,用于根据光束的总光谱数据和预设波段的光束的功率,生成光束的总功率。The generating
进一步地,多个波段的光谱数据中若干波段的光谱数据为对数光谱数据,剩余波段的光谱数据为线性光谱数据,Further, among the spectral data of multiple bands, the spectral data of several bands are logarithmic spectral data, and the spectral data of the remaining bands are linear spectral data,
拼接单元402,还用于将线性光谱数据转换为转换对数光谱数据,并在对数光谱数据和转换对数光谱数据中选取任意一个光谱数据作为基准对数光谱数据。The
拼接单元402,还用于在剩下的对数光谱数据和转换对数光谱数据中,选取对应的波段与基准对数光谱数据的波段有重合的光谱数据,作为待拼接对数光谱数据。The
拼接单元402,还用于基于基准对数光谱数据和待拼接对数光谱数据的重合波段,按照预设算法计算得到连接波长。The
拼接单元402,还用于在基准对数光谱数据和待拼接对数光谱数据中,分别获取与连接波长相应的基准对数强度值和待拼接对数强度值。The
拼接单元402,还用于将待拼接对数强度值减去基准对数强度值,得到偏差值,并根据偏差值,将待拼接对数光谱数据中的全部对数强度值减去偏差值,以将待拼接对数光谱数据和基准对数光谱数据在连接波长处拼接在一起。The
拼接单元402,还用于将拼接后的基准对数光谱数据和待拼接对数光谱数据作为新的基准对数光谱数据,并基于新的基准对数光谱数据,执行在剩下的对数光谱数据和转换对数光谱数据中,选取对应的波段与基准对数光谱数据的波段有重合的光谱数据,作为待拼接对数光谱数据的步骤,直至将多个波段的光谱数据全部拼接在一起,得到光束的总对数光谱数据。The
拼接单元402,还用于将光束的总对数光谱数据进行转换,得到光束的总线性光谱数据。The
进一步地,生成单元405,还用于将光束的总线性光谱数据进行求和,得到光束的光谱总强度。Further, the
生成单元405,还用于在光束的总线性光谱数据中选取预设波段的光谱数据并进行求和,得到预设波段的光束的光谱强度。The
生成单元405,还用于根据光束的光谱总强度、预设波段的光束的光谱强度和预设波段的光束的功率,生成光束的总功率。The generating
进一步地,电子设备还包括:Further, the electronic equipment also includes:
计算单元406,与生成单元405相连,用于将光束的光谱总强度除以光束的总功率,得到光束的光谱总强度和光束的总功率之间的比例值。The calculating
计算单元406,还用于将光束的光谱总强度中的全部的强度值除以比例值,得到光束的光谱功率密度数据。The
绘图单元407,与生成单元405和计算单元406相连,用于根据光束的总对数光谱数据、光束的总线性光谱数据和光束的光谱功率密度数据进行绘制,分别得到光束的总对数光谱图、光束的总线性光谱图和光束的功率密度分布图。The
进一步地,生成单元405,还用于按照如下公式根据光束的光谱总强度、预设波段的光束的光谱强度和预设波段的光束的功率,生成光束的总功率:Further, the generating
式中,P总表示光束的总功率,S总表示光束的光谱总强度,S表示预设波段的光束的光谱强度,P表示预设波段的光束的功率。In the formula, P total represents the total power of the beam, S total represents the total spectral intensity of the beam, S represents the spectral intensity of the beam in the preset band, and P represents the power of the beam in the preset band.
在本发明实施例中,通过多个光谱测量单元直接测量得到多个波段的光谱数据,通过滤波单元对光源进行滤波得到预设波段的光束,并通过功率测量单元直接测量该预设波段的光束,然后通过直接测量得到的多个波段的光谱数据和预设波段的功率计算得到光源的总功率,而不需利用不同波段的功率计对光源进行测量并求和得到光源的总功率,从而避免了不同波段的功率计的标定方法不同所引起的误差,进而提高了测量超连续谱光源的总功率的精确度。In the embodiment of the present invention, the spectral data of multiple bands is directly measured by multiple spectral measurement units, the light source is filtered by the filtering unit to obtain the beam of the preset band, and the beam of the preset band is directly measured by the power measurement unit , and then calculate the total power of the light source by directly measuring the spectral data of multiple bands and the power of the preset bands, without using power meters in different bands to measure the light source and sum to obtain the total power of the light source, thereby avoiding The error caused by different calibration methods of power meters in different bands is eliminated, and the accuracy of measuring the total power of supercontinuum light sources is improved.
需要说明的是,对于前述的各方法实施例,为了简便描述,故将其都表述为一系列的动作组合,但是本领域技术人员应该知悉,本发明并不受所描述的动作顺序的限制,因为依据本发明,某些步骤可以采用其他顺序或者同时进行。其次,本领域技术人员也应该知悉,说明书中所描述的实施例均属于优选实施例,所涉及的动作和模块并不一定都是本发明所必须的。It should be noted that, for the sake of simplicity of description, the aforementioned method embodiments are expressed as a series of action combinations, but those skilled in the art should know that the present invention is not limited by the described action sequence. Because of the present invention, certain steps may be performed in other orders or simultaneously. Secondly, those skilled in the art should also know that the embodiments described in the specification belong to preferred embodiments, and the actions and modules involved are not necessarily required by the present invention.
在上述实施例中,对各个实施例的描述都各有侧重,某个实施例中没有详述的部分,可以参见其他实施例的相关描述。In the foregoing embodiments, the descriptions of each embodiment have their own emphases, and for parts not described in detail in a certain embodiment, reference may be made to relevant descriptions of other embodiments.
以上为本发明所提供的功率测量方法和电子设备的描述,对于本领域的一般技术人员,依据本发明实施例的思想,在具体实施方式及应用范围上均有改变之处,综上,本说明书内容不应理解为对本发明的限制。The above is the description of the power measurement method and electronic equipment provided by the present invention. For those of ordinary skill in the art, according to the idea of the embodiment of the present invention, there are changes in the specific implementation and application range. In summary, this The content of the description should not be construed as limiting the present invention.
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Title |
---|
"用于探测器中红外绝对光谱响应度测量的激光源";赵坤 等;《红外与激光工程》;第45卷(第7期);第0705005-1-0705005-7页 * |
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