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          1. Resources
          2. Technical Notes
          3. Optics
          4. Optical Materials

          Technical Note:
          Optical Materials

          Newport offers a wide variety of spherical and aspherical lenses made from BK 7, UV grade fused silica, Infrared grade Calcium Fluoride (CaF2), Magnesium Fluoride (MgF2), AMTR and Zinc Selenide materials. For applications in the visible and infrared up to about 2.1 µm, BK 7 offers excellent performance at a good value. In the ultraviolet down to 195 nm, UV fused silica is a good choice. UV fused silica also has excellent transmission in the visible and infrared up to about 2.1 µm, better homogeneity, and a lower coefficient of thermal expansion than BK 7. CaF2 and MgF2 are excellent choices for deep UV or infrared applications—for custom applications, Newport can provide quotes on a build-to-print basis.

          For common optical materials, this technical note offers specifications for important basic parameters such as index of refraction, transmission across various wavelength ranges, reflectance, Abbe Number, coefficient of thermal expansion, conductivity, heat capacity, density, Knoop hardness, and Young's modulus.

          Also see Optical Material Properties, for additional information.

          BK 7

          BK 7 is one of the most common borosilicate crown glasses used for visible and near infrared optics. Its high homogeneity, low bubble and inclusion content, and straightforward manufacturability make it a good choice for transmissive optics. BK7 is also relatively hard and shows good scratch resistance. The transmission range for BK 7 is 380–2100 nm. It is not recommended for temperature sensitive applications, such as precision mirrors.

          N-BK7 transmittance (%) vs. wavelength (nm) with 4% reflection from both sides
          N-BK7 transmittance (%) in the UV vs. wavelength (nm) with 4% reflection from both sides

          UV Grade Fused Silica

          UV Grade Fused Silica is synthetic amorphous silicon dioxide of extremely high purity. This non-crystalline, colorless silica glass combines a very low thermal expansion coefficient with good optical qualities, and excellent transmittance in the ultraviolet region down to 195 nm. Transmission and homogeneity exceed those of crystalline quartz without the problems of orientation and temperature instability inherent in the crystalline form. Fused silica is ideally used with high-energy lasers due to its high energy damage threshold. UV fused silica also has excellent transmission in the visible and infrared region up to approximately 2.1 µm, and a low content of inclusions with high refractive index homogeneity. Fused silica is used for both transmissive and reflective optics, especially where high laser damage threshold is required.

          FUSEDSIL-S

          CaF2

          Calcium Fluoride is a cubic single crystal material grown using the vacuum Stockbarger Technique with good vacuum UV to infrared transmission. CaF2 has a wide spectral range and is an excellent choice for deep UV to infrared applications because of its non-birefringent properties. CaF2 has a transmission above 90% between 0.25 and 7µm, and is commonly used for excimer laser optics due to its low absorption and high damage threshold. Material for IR use is grown using naturally mined fluorite, at much lower cost. CaF2 has very poor thermal properties with its high coefficient of thermal expansion, and should be avoided in high operating temperature environment. Calcium fluoride can be used without an Anti-Reflection coating due to its low index of refraction.

          Note that this material is mildly hydroscopic. If used under normal operating conditions, no pitting is expected. However, it is not recommended for water immersion applications.

          CAF2CURV-S

          MgF2

          Magnesium Fluoride is a positive birefringent crystal grown using the vacuum Stockbarger Technique with good vacuum UV to infrared transmission. It is typically oriented with the c axis parallel to the optical axis to reduce birefringent effects. MgF2 is another excellent choice for deep UV to infrared regions, with good transmission range from 0.15 µm to 6.5 µm, and its proven use in fluorine environments make it ideal for lenses, windows, and polarizers for Excimer lasers. MgF2 is resistant to the thermal and mechanical shock, and has higher energy damage threshold. MgF2 is one of the lowest index infrared materials, which usually doesn’t require anti-reflection coating. MgF2 is extremely durable compared to other materials which are transparent from the UV to the IR spectrum. MgF2 is an ideal choice for many biological and military imaging applications that require wide broadband laser pulses.

          Note that this material is mildly hydroscopic. If used under normal operating conditions, no pitting is expected. However, it is not recommended for water immersion applications.

          MGF2CURV-S

          Crystal Quartz

          Crystal Quartz is a positive uniaxial birefringent single crystal grown using a hydrothermal process. It has good transmission from the vacuum UV to the near infrared. Due to its birefringent nature, crystal quartz is commonly used for wave plates.

          QUARTZCU-S

          Borofloat®

          Borofloat® is a borosilicate glass with a low coefficient of thermal expansion. It is mainly used for non-transmissive optics, such as mirrors, due to its low homogeneity and high bubble content.

          Zerodur®

          Zerodur® is a glass ceramic material that has a coefficient of thermal expansion approaching zero, as well as excellent homogeneity of this coefficient throughout the entire piece. This makes Zerodur ideal for mirror substrates where extreme thermal stability is required. Zerodur should not be used for transmissive optics due to inclusions in the material.

          ZnSe

          Zinc selenide is a chemically vapor deposited material commonly used in thermal imaging and medical systems. ZnSe is an excellent choice for IR lens with its broad wavelength range (600nm- 16 µm). ZnSe has a high index of refraction which normally requires an anti-reflection coating to achieve high transmission. ZnSe is relatively soft with low scratch resistance thus not recommended for use in harsh environment. Extra caution is required during cleaning, handling, and mounting. ZnSe is the best choice for optics used in high power CO2 laser systems due to its low absorption coefficient and high resistance to thermal shock

          Properties of Optical Materials

          Material Abbe Number
          vd
          Coefficient of Thermal Expansion
          (10-6/°C)
          Conductivity
          (W/m°C)
          Heat Capacity
          (J/gm°C)
          Density at 25°C
          (gm/cm3)
          Knoop Hardness
          (kg/mm2)
          Young's Modulus
          (GPa)
          BK 7 64.17 7.1 1.114 0.858 2.51 610 81.5
          SF 2 33.85 8.4 0.735 0.498 3.86 410 55
          UV Fused Silica 67.8 0.52 1.38 0.75 2.202 600 73
          CaF2 94.96 18.85 9.71 0.85 3.18 158 75.8
          MgF2 106.18 13.7 || to c axis
          8.48 ⊥ to c axis
          21 || to c axis
          30 to ⊥ c axis
          1.024 3.177 415 138.5
          Crystal Quartz 69.87 7.1 to || c axis
          13.2 ⊥ to c axis
          10.4 || to c axis
          6.2 ⊥ to c axis
          0.74 2.649 740 97 || to c axis
          76.5 ⊥ to c axis
          Borofloat® 65.41 3.25 1.2 0.83 2.2 480 64
          Zerodur® 56.09 0 ± 0.1 1.46 0.80 2.53 620 90.3
          ZnSe 84.45 7.6 18.0 0.399 5.27 105 70

          Common Optical Material Properties

          Material Transmission Range Cost Features
          BK 7 380–2100 nm Low High transmission for visible to near infrared applications, the most common optical glass
          UV Fused Silica (UVFS) 195–2100 nm Moderate Excellent homogeneity and low thermal expansion, high laser damage resistance
          CaF2 170–8000 nm High High transmission for deep UV to infrared applications
          MgF2 150–6500 nm High Birefringent material, excellent for use in the deep UV to infrared
          ZnSe 600–16000 nm High Excellent choice for IR lens due to its broad wavelength range. Perfect candidate to use with high power infrared laser due to its low absorption coefficient.

          Index of Refraction

          Wavelength
          (nm)
          Source BK 7 SF 2 UV Fused Silica CaF2 MgF2
          no
          MgF2
          ne
          Crystal Quartz
          no
          Crystal Quartz
          ne
          193 ArF excimer laser 1.65528 1.52127 1.56077 1.50153 1.42767 1.44127 1.66091 1.67455
          244 Ar-Ion laser 1.58265 1.98102 1.51086 1.46957 1.40447 1.41735 1.60439 1.61562
          248 KrF excimer 1.57957 1.93639 1.50855 1.46803 1.40334 1.41618 1.60175 1.61289
          257 Ar-Ion laser 1.57336 1.86967 1.50383 1.46488 1.40102 1.41377 1.59637 1.60731
          266 Nd:YAG laser 1.56796 1.82737 1.49968 1.46209 1.39896 1.41164 1.59164 1.60242
          308 XeCl excimer laser 1.55006 1.73604 1.48564 1.45255 1.39188 1.40429 1.57556 1.58577
          325 HeCd laser 1.54505 1.71771 1.48164 1.44981 1.38983 1.40216 1.57097 1.58102
          337.1 N2 laser 1.54202 1.70749 1.47919 1.44813 1.38858 1.40085 1.56817 1.57812
          351 XeF excimer laser 1.53896 1.69778 1.47672 1.44642 1.38730 1.39952 1.56533 1.57518
          351.1 Ar-Ion laser 1.53894 1.69771 1.47671 1.44641 1.38729 1.39951 1.56531 1.57516
          354.7 Nd:YAG laser 1.53821 1.69548 1.47612 1.44601 1.38699 1.39920 1.56463 1.57446
          363.8 Ar-Ion laser 1.53649 1.69029 1.47472 1.44504 1.38626 1.39844 1.56302 1.57279
          404.7 Mercury arc, h line 1.53023 1.67263 1.46961 1.44151 1.38360 1.39567 1.55714 1.56670
          416 Kr-Ion laser 1.52885 1.66893 1.46847 1.44072 1.38301 1.39505 1.55583 1.56535
          435.8 Mercury arc,g line 1.52669 1.66331 1.46670 1.43949 1.38207 1.39408 1.55379 1.56323
          441.6 HeCd laser 1.52611 1.66184 1.46622 1.43916 1.38183 1.39382 1.55324 1.56266
          457.9 Ar-Ion laser 1.52461 1.65807 1.46498 1.43830 1.38118 1.39314 1.55181 1.56119
          465.8 Ar-Ion laser 1.52395 1.65641 1.46443 1.43792 1.38088 1.39284 1.55118 1.56053
          472.7 Ar-Ion laser 1.52339 1.65505 1.46397 1.43760 1.38064 1.39258 1.55065 1.55998
          476.5 Ar-Ion laser 1.52309 1.65432 1.46372 1.43744 1.38051 1.39245 1.55036 1.55969
          480 Cadmium arc, F’ line 1.52283 1.65367 1.46350 1.43728 1.38040 1.39233 1.55011 1.55943
          486.1 Hydrogen arc, F line 1.52238 1.65258 1.46313 1.43703 1.38020 1.39212 1.54968 1.55898
          488 Ar-Ion laser 1.52224 1.65225 1.46301 1.43695 1.38014 1.39206 1.54955 1.55885
          496.5 Ar-Ion laser 1.52165 1.65083 1.46252 1.43661 1.37988 1.39179 1.54898 1.55826
          501.7 Ar-Ion laser 1.52130 1.65000 1.46223 1.43641 1.37973 1.39163 1.54865 1.55792
          510.6 Cu vapor laser 1.52073 1.64865 1.46176 1.43609 1.37948 1.39137 1.54810 1.55735
          514.5 Ar-Ion laser 1.52049 1.64808 1.46156 1.43595 1.37937 1.39126 1.54787 1.55711
          532 Nd:YAG laser 1.51947 1.64570 1.46071 1.43537 1.37892 1.39079 1.54689 1.55610
          543.5 HeNe laser 1.51886 1.64427 1.46019 1.43502 1.37865 1.39051 1.54630 1.55549
          546.1 Mercury arc, e line 1.51872 1.64397 1.46008 1.43494 1.37859 1.39044 1.54617 1.55535
          578.2 Cu vaport laser 1.51720 1.64053 1.45880 1.43408 1.37792 1.38974 1.54470 1.55383
          587.6 Helium arc, d line 1.51680 1.63963 1.45846 1.43385 1.37774 1.38956 1.54431 1.55343
          589.3 Sodium arc, D line 1.51673 1.63947 1.45840 1.43381 1.37771 1.38952 1.54424 1.55336
          594.1 HeNe laser 1.51653 1.63904 1.45824 1.43370 1.37762 1.38943 1.54405 1.55316
          611.9 HeNe laser 1.51584 1.63752 1.45765 1.43331 1.37732 1.38911 1.54337 1.55247
          628 Ruby laser 1.51526 1.63626 1.45716 1.43298 1.37706 1.38884 1.54281 1.55188
          632.8 HeNe laser 1.51509 1.63590 1.45702 1.43289 1.37698 1.38876 1.54264 1.55171
          635 Laser diode 1.51501 1.63574 1.45695 1.43284 1.37695 1.38873 1.54257 1.55164
          643.8 Cadmium arc, C' line 1.51472 1.63512 1.45671 1.43268 1.37682 1.38859 1.54228 1.55134
          647.1 Kr-Ion laser 1.51461 1.63489 1.45661 1.43262 1.37677 1.38854 1.54218 1.55123
          650 Laser diode 1.51452 1.63469 1.45653 1.43257 1.37673 1.38850 1.54209 1.55114
          656.3 Hydrogen arc, C line 1.51432 1.63427 1.45637 1.43246 1.37664 1.38840 1.54189 1.55093
          670 Laser diode 1.51391 1.63340 1.45601 1.43223 1.37646 1.38821 1.54148 1.55051
          676.4 Kr-Ion laser 1.51372 1.63301 1.45585 1.43212 1.37637 1.38812 1.54130 1.55032
          694.3 Ruby laser 1.51322 1.63198 1.45542 1.43185 1.37615 1.38789 1.54080 1.54981
          750 Laser diode 1.51184 1.62922 1.45424 1.43109 1.37553 1.38724 1.53943 1.54839
          780 Laser diode 1.51118 1.62796 1.45367 1.43074 1.37524 1.38693 1.53878 1.54771
          830 Laser diode 1.51020 1.62613 1.45282 1.43023 1.37480 1.38647 1.53779 1.54668
          850 Laser diode 1.50984 1.62548 1.45250 1.43004 1.37464 1.38630 1.53742 1.54630
          852.1 Cesium arc, s line 1.50980 1.62541 1.45247 1.43002 1.37462 1.38628 1.53739 1.54626
          905 Laser diode 1.50892 1.62387 1.45168 1.42957 1.37422 1.38586 1.53648 1.54532
          980 Laser diode 1.50779 1.62202 1.45067 1.42902 1.37371 1.38533 1.53531 1.54409
          1014 Mercury arc, t line 1.50731 1.62128 1.45024 1.42879 1.37350 1.38510 1.53481 1.54357
          1053 Nd:YLF laser 1.50678 1.62049 1.44976 1.42854 1.37326 1.38485 1.53425 1.54299
          1060 Nd:Glass laser 1.50669 1.62035 1.44968 1.42850 1.37322 1.38480 1.53415 1.54288
          1064 Nd:YAG laser 1.50663 1.62028 1.44963 1.42848 1.37319 1.38478 1.53410 1.54282
          1300 Laser diode 1.50370 1.61644 1.44692 1.42721 1.37188 1.38338 1.53094 1.53950
          1320 Nd:YAG laser 1.50346 1.61616 1.44669 1.42711 1.37177 1.38327 1.53068 1.53922
          1550 Laser diode 1.50065 1.61312 1.44402 1.42602 1.37052 1.38194 1.52761 1.53596
          1970.1 Mercury arc 1.49495 1.60780 1.43852 1.42401 1.36803 1.37928 1.52138 1.52932
          2100 Ho:YAG laser 1.49296 1.60608 1.43659 1.42334 1.36718 1.37837 1.51924 1.52703
          2325.4 Mercury arc 1.48921 1.60291 1.43293 1.42212 1.36559 1.37667 1.51524 1.52277
          2940 Er:YAG laser 1.47670 1.59273 1.42065 1.41827 1.36051 1.37123 1.50246 1.50908

          Transmittance of Optical Materials

          These graphs compare the transmission of standard optical materials. The transmission values listed here are equivalent to "external transmittance" and takes into consideration the reflectances you get from uncoated optical elements.

          EG-pg15-8a
          Transmission of 10 mm thick fused silica of different grades, and crown glass windows.
          EG-pg15-8b
          Transmittance of IR optical materials.
          EG-pg15-9a
          Transmittance of UV-IR materials.
          EG-pg15-9b
          Transmittance of VIS-NIR materials.

          Reflectance of Optical Materials

          All metal reflectors deteriorate slowly in polluted atmosphere. Cumulative exposure to intense ultraviolet radiation also affects performance; overheating of the reflective surface will destroy the reflector.

          EG-pg15-10a
          Typical near normal incidence reflectance of freshly deposited Al, AlMgF2, AlSiO, and Au.

          The AlMgF2 coating has been optimized for performance in the near UV.

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      • '); $.ajax({ type: "GET", url: url, data: {orderNumber: orderNumber, zipCode: zipCode}, success: function (result) { $(".ajaxLoading-bg, .ajaxLoading-img").remove(); if (result.length > 0) { if (result[0].name == 'Success') { $('#checkOrderStatusForm').attr('action', ACC.config.contextPath + '/guest/getOrderStatus'); $('#checkOrderStatusForm').submit(); } if (result[0].name == 'Failure') { $('#checkOrderStatusMessage').after('' + result[0].value + ''); } } }, error: function (result) { $('#checkOrderStatusMessage').after('' + result[0].value + ''); } }); } else { event.preventDefault(); } }); }); function paywallEmail(newportResourceValue, newportResourceTypeValue, productCodeValue, pageOwnerValue) { $('#payWallForm').remove(); var payWallForm = document.createElement("form"); document.body.appendChild(payWallForm); payWallForm.id = "payWallForm"; payWallForm.method = "POST"; payWallForm.action = "/paywallemail"; var newportResource = document.createElement("input"); newportResource.name="newportResource"; newportResource.value = newportResourceValue; newportResource.type = "hidden"; payWallForm.appendChild(newportResource); var newportResourceType = document.createElement("input"); newportResourceType.name="npResourceType"; newportResourceType.value = newportResourceTypeValue; newportResourceType.type = "hidden"; payWallForm.appendChild(newportResourceType); var productCode = document.createElement("input"); productCode.name="productCode" productCode.value = productCodeValue; productCode.type = "hidden"; payWallForm.appendChild(productCode); var pageOwner = document.createElement("input"); pageOwner.name="pageOwner" pageOwner.value = pageOwnerValue; pageOwner.type = "hidden"; payWallForm.appendChild(pageOwner); var pURL = ACC.config.contextPath + "/login/paywallemail"; $.ajax({ type: 'POST', url: pURL, data: $("#payWallForm").serialize(), success: function (result) { var downloadUrl = result[0].value; var cookieCreated = result[1].value; console.log("DownloadUrl - " + downloadUrl); console.log("CookieCreated - " + cookieCreated); window.open(downloadUrl); } }); } function validateResourceDownloadForm() { // added this line of code for lazy loading $('body').prepend('
        '); var favouriteURL = $('#favourite_link').val(); console.log("validateResourceDownloadForm"); $("#newportResource").val($('#newportResourcePK').val()); $('#productCode').val($(this).data('productCode')); $('#pageOwner').val($(this).data('pageOwner')); $('#npResourceType').val($(this).data('newportResourceType')); $.ajax({ type: $("#resourceDownloadForm").attr('method'), url: $("#resourceDownloadForm").attr('action'), data: $("#resourceDownloadForm").serialize(), async:false, success: function (result) { var downloadUrl = result[0].value; pardotOptInResourceDownloadForm('firstName', 'lastName', 'emailAddress', 'companyName', '', 'contactCountry', 'contactShipState', '', result[3].value); if ($('#npResourceType').val() == 'videoUrl') { } else { window.open(downloadUrl, '_blank'); } $(".ajaxLoading-bg, .ajaxLoading-img").remove(); $('#resourceDownload').modal('hide'); setTimeout(function () { location.reload(true); }, 1000); }, error: function (data) { console.log('An error test occurred.'); console.log(data); }, }); } function isValidCaptchaResponse() { try { var vCaptcha = $('#v-captcha').val(); var grecaptcha = $('#g-recaptcha-response').val(); var vCaptchStatus = $('#captchaStatus').val(); if (vCaptcha != undefined && vCaptcha.length > 0) { return true; } if (grecaptcha != undefined && grecaptcha.length > 0) { return true; } else { return vCaptchStatus == "true"; } } catch (err) { return vCaptchStatus == "true"; } } function validateSignInForm() { // added this line of code for lazy loading $('body').prepend('
        '); var favouriteURL = $('#favourite_link').val(); var vURL = ACC.config.contextPath + "/login/headerlogin"; $ .ajax({ type: 'POST', url: vURL, data: $("#signInForm").serialize(), success: function (result) { //First, remove the spinner $(".ajaxLoading-bg, .ajaxLoading-img").remove(); [] var nameStr = result[0].name; var valueStr = result[0].value; var pardotSignInUrl = result[1].value; var loginRedirectUrl; if (nameStr == "Success") { if(result.length > 2) { loginRedirectUrl = result[2].value; if(loginRedirectUrl.endsWith("/checkout")) { window.location.href = loginRedirectUrl; return; } } if (favouriteURL != '') { $.post(favouriteURL, function (result) { window.location.href = window.location.href; }); } else { window.location.href = window.location.href.replace(window.location.hash, ""); } if ($('#newportResourcePK').val() != '') { paywallEmail($('#newportResourcePK').val(), $('#productCode').val(), $('#pageOwner').val()); } var emailStr = "emailAddress=" + $('#j_username').val(); doPardotSignIn(emailStr, pardotSignInUrl); } else if (nameStr == "SuccesswithCartMerge") { doPardotSignIn(emailStr, pardotSignInUrl); createMergeCartCookie(); window.location.href = window.location.href; } else if (nameStr == "/cart/checkout") { doPardotSignIn(emailStr, pardotSignInUrl); window.location.href = ACC.config.contextPath + nameStr; } else if (nameStr == "/cart/checkoutwithCartMerge") { doPardotSignIn(emailStr, pardotSignInUrl); createMergeCartCookie() window.location.href = "/cart"; } else if (nameStr == "/checkout/single/quotesummary") { doPardotSignIn(emailStr, pardotSignInUrl); window.location.href = nameStr; } else if (nameStr == "/checkout/single/quotesummarywithCartMerge") { doPardotSignIn(emailStr, pardotSignInUrl); createMergeCartCookie() window.location.href = "/cart"; } else if (nameStr == "redirect:/welcome") { doPardotSignIn(emailStr, pardotSignInUrl); window.location.href = "/welcome"; } else if (nameStr == "maxpasswordCount") { $('#j_username').next('span').remove(); var resetPwdLink = $('#resetPwdLink').val(); $("#PasswordReset").val(resetPwdLink); $('#j_username').after('Too many failed sign-in attempts. Please reset your password using the link below to unlock your account.'); } else if (nameStr == "email not found") { $('#j_username').next('span').remove(); $('#j_username').after('Entered email address or password is wrong'); } else if (nameStr == "Bad Password") { $('#j_username').next('span').remove(); $('#j_username').after('Entered email address or password is wrong'); } else if (nameStr == "modal") { $('#check_availability_modal').html(valueStr) $('#check_availability_modal').modal(); } else { $('#j_username').next('span').remove(); $('#j_username').after('Entered email address or password is wrong'); } } }); } function createMergeCartCookie() { createCookie("mergeCart", "true"); } function removeMergeCartCookie() { removeCookie("mergeCart"); } function getCookie(name) { var value = "; " + document.cookie; var parts = value.split("; " + name + "="); if (parts.length == 2) return parts.pop().split(";").shift(); } function createCookie(name, value) { document.cookie = name + "=" + value + ";path=/"; } function removeCookie(name) { document.cookie = name + "=;expires=Thu, 01 Jan 1970 00:00:01 GMD;path=/"; } function doPardotSignIn(emailStr, pardotSignInUrl) { $.ajax({ type: "POST", url: pardotSignInUrl, data: emailStr, success: function (data) { }, error: function (data) { //Do Nothing; } }); } function pardotOptInResourceDownloadForm(firstName, lastName, emailId, companyId, phoneId, countryCodeId, stateCodeId, zipcodeId, title) { var siteId = $("#cmsSiteUid").val(); var cbPardotOptIn = $('#cbPardotOptIn').prop('checked'); var pardotOptInUrls = $('#pardotOptInUrls').val(); var pardotUrlArr = pardotOptInUrls.split(','); var pardotUrl = (cbPardotOptIn ? pardotUrlArr[0] : pardotUrlArr[1]); var cbPardotOptInParam = (cbPardotOptIn ? 'YES' : 'NO'); if (!pardotUrl) { return; } var email = $('#' + emailId).val().trim(); var fName= $('#' + firstName).val().trim(); var lname = $('#' + lastName).val().trim(); var dataStr = 'emailAddress=' + email + '&firstName=' + encodeURIComponent(fName) + '&lastName=' + encodeURIComponent(lname); if(companyId) { var company = $('#' + companyId).val(); dataStr += ( '&companyName=' + encodeURIComponent(company) ); } if (phoneId) { var phone = $('#' + phoneId).val(); dataStr += ( '&phoneNumber=' + encodeURIComponent(phone) ); } if (countryCodeId) { var country = $('#' + countryCodeId).val(); var pardotCountry = (country == "US" ? "USA" : ""); dataStr += ( '&country123=' + encodeURIComponent(pardotCountry) ); } if (stateCodeId) { var state = $('#' + stateCodeId).val(); dataStr += ( '&state=' + encodeURIComponent(state) ); } if (zipcodeId) { var zipcode = $('#' + zipcodeId).val(); if (zipcode && zipcode.length > 0) { dataStr += ( '&postalCode=' + encodeURIComponent(zipcode) ); } } if (siteId == 'esi') { dataStr += ( '&cbPardotOptIn=' + cbPardotOptInParam ); } if (siteId == 'newport') { dataStr += ( '&Document_Downloaded=' + title ); } buildResourceDownloadPardotIframe(pardotUrl, dataStr); } function buildResourceDownloadPardotIframe(pardotUrl, dataStr) { if (pardotUrl) { var iframeStr = ""; $('#pardotIframeIdResourceDownload').html(iframeStr); } } $(document).ready(function () { //Show cart merge modal if requested if(getCookie("mergeCart") === "true") { removeMergeCartCookie(); $("#cartMergedSuccess").modal(); $("#mergedMsg").html("Recovered cart items from your last sign-in have been added to your current cart. Please review your items and quantities carefully prior to checkout."); $('#popupClose').click(function () { $('.ajaxLoading-bg').show(); $('.ajaxLoading-img').show(); }); $('#cartMergeCloseIcon').click(function () { $('.ajaxLoading-bg').show(); $('.ajaxLoading-img').show(); }); } $('a[href="' + ACC.config.contextPath + '/guest/checkOrderStatus"]').click(function (event) { event.preventDefault(); $('#check_order_status_modal').modal(); }); // added method for removing vslidation onBlur $.validate({ form: '#forgottenPwdForm', validateOnBlur: false, showHelpOnFocus: false, addSuggestions: true }); $("#forgottenPwdForm").submit(function (event) { event.preventDefault(); validateForgotpswdForm(); }); //This will show alert popups if (''.length > 0) { // if(true) { $.ajax({ type: "GET", url: "/alert", data: {title: "Important Message", message: ""}, // parameters sync: true, success: function (result) { if (result.length > 0) { $('#alert_modal').html(result) $('#alert_modal').modal(); } else { //Do Nothing } }, error: function (result) { alert("error! " + result); } }); } }); //added the method to avoid the conflict between checkout sign in and header sign in on cart page. function clearRedirectValue() { $(".form-redirect").attr("value", "") $("input[id$='demo-field']").each(function () { if ($(this).attr('type').eq("password")) { $(this).css('display', 'block') $(this).val(""); } if ($(this).attr('type').eq("text")) { $(this).css('display', 'none') $(this).val(""); } }); $('[id^="showpasscheckbox"]').attr('checked', false); } // TODO function validateForgotpswdForm() { if($("#forgottenPwdForm").isValid()) { var vusername = document.getElementById("email").value; var resetMsg = $('#resetMsg').val(); var vURL = ACC.config.contextPath + "/login/pw/request"; $ .ajax({ type: 'post', url: vURL, data: $("#forgottenPwdForm").serialize(), success: function (data) { $("#accountPasswordReset").hide(); $("#accountPasswordResetSuccess").modal(); $(".msg").html(resetMsg); }, error: function (jqXHR, exception) { $(".msg").html("Entered email address or password is wrong"); } }); } } function validatePassword() { $("#checkPasswordValidOrNot").addClass("help-block form-error"); $("#checkPasswordValidOrNot").hide(); } function validateEmail() { $("#forgotEmailMsg").addClass("help-block form-error"); $("#forgotEmailMsg").hide(); } $('.modal').on('hidden.bs.modal', function () { /* $(this).find('form')[0].reset(); */ $('#checkPasswordValidOrNot').hide(); }); $('#PasswordReset').on('click', function (event) { var signupEmail = $("#j_username").val(); $('#email').val(signupEmail); }); $('#j_username').on('focusout', function () { var text = $.trim($(this).val()); this.value = ""; this.value = text; }); function registrationSalesForceSubmit() { var industryforsalesforce = ''; var industryforsalesforcearray = industryforsalesforce.split(','); var industry = ''; if (industry == 'Aerospace & Defense') { industry = industryforsalesforcearray[1]; } if (industry == 'Research & Education') { industry = industryforsalesforcearray[0]; } if (industry == 'Life & Health Science') { industry = industryforsalesforce[3]; } if (industry == 'Microelectronics') { industry = industryforsalesforcearray[2]; } if (industry == 'Industrial Manufacturing') { industry = industryforsalesforcearray[4]; } // modified for sales force value var residential = ''; if (residential == 'false') { residential = 'No'; } else { residential = 'Yes'; } var reseller = ''; if (reseller == 'false') { reseller = 'No'; } else { reseller = 'Yes'; } var state = ''; if (state != '') { var statearray = state.split("-"); state = statearray[1]; } var country = ''; if (country == 'US' || country == 'CA') { } else { state = ""; } var title = ''; if (title != '') { var myTitle = title; title = myTitle.substring(0, 1).toUpperCase() + myTitle.substring(1); } var usersalutation = ''; var userfirstname = ''; var userlastname = ''; var useremail = ''; var userphone = ''; var userurl = ''; var userstate = ''; var userstreet = ''; var usercity = ''; var usercompany = ''; var userzip = ''; var usercountry = ''; var userprimarymarket = ''; var userdescription = ''; var userleadsource = ''; var useroid = ''; var usercurrency = ''; var userbusinessunit = ''; var userjobtitle = ''; var userrecordtype = ''; var userregion = ''; var userbusinessgroup = ''; $ .ajax({ type: "POST", url: '', data: usersalutation + '=' + title + '&' + userfirstname + '=' + '' + '&' + useremail + '=' + '' + '&' + userphone + '=' + '' + '&' + userlastname + '=' + '' + '&' + userurl + '=' + '' + '&' + userstate + '=' + state + '&' + userstreet + '=' + '' + '&' + usercity + '=' + '' + '&' + usercompany + '=' + '' + '&' + userzip + '=' + '' + '&' + usercountry + '=' + '' + '&' + userprimarymarket + '=' + encodeURIComponent(industry) + '&' + userdescription + '=' + encodeURIComponent('Lead was generated through web registration form. Customer provided account number: ' + '' + '\n' + 'isResedential: ' + residential + '\n' + 'isReseller: ' + reseller) + '&' + userleadsource + '=' + '' + '&' + useroid + '=' + '' + '&' + usercurrency + '=' + '' + '&' + userbusinessunit + '=' + '' + '&' + userbusinessgroup + '=' + '' + '&' + userjobtitle + '=' + '' + '&' + userrecordtype + '=' + '' + '&' + userregion + '=' + '' }); }