Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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58492 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }M_{2}\phi_{1}^{3}$ | 1.4536 | 1.6428 | 0.8849 | [X:[1.3305], M:[0.9957, 0.9957], q:[0.485, 0.5109], qb:[0.5021, 0.4934], phi:[0.3348]] | [X:[[0, 2]], M:[[0, 3], [0, 3]], q:[[-1, 15], [-1, -3]], qb:[[1, -6], [1, 0]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{1}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}^{2}$ | ${}$ | -3 | t^2.94 + t^2.96 + 2*t^2.99 + t^3.04 + t^3.94 + t^3.97 + t^3.99 + t^4.02 + t^4.04 + t^4.94 + t^4.97 + t^5.02 + t^5.05 + t^5.45 + t^5.47 + t^5.5 + t^5.52 + t^5.87 + t^5.9 + 2*t^5.92 + 2*t^5.95 + 3*t^5.97 - 3*t^6. + t^6.03 + t^6.45 + t^6.48 + t^6.5 + t^6.53 + t^6.87 + 2*t^6.9 + 3*t^6.93 + 4*t^6.95 + 4*t^6.98 + t^7. + 2*t^7.03 + t^7.06 + t^7.38 + t^7.46 + t^7.53 + t^7.61 + 2*t^7.88 + 3*t^7.9 + 3*t^7.93 + 4*t^7.96 + 4*t^7.98 + 3*t^8.01 + 2*t^8.03 + 2*t^8.06 + t^8.09 + t^8.38 + t^8.41 + 2*t^8.43 + 2*t^8.46 + t^8.48 - t^8.54 - t^8.56 - t^8.59 + t^8.81 + t^8.83 + 2*t^8.86 + 3*t^8.88 + 5*t^8.91 + 2*t^8.96 - 3*t^8.99 - t^4./y - t^5.01/y - t^6.94/y - t^6.97/y - (2*t^6.99)/y - t^7.04/y - t^7.94/y - t^7.97/y - (2*t^8.)/y - t^8.05/y + t^8.9/y + (2*t^8.92)/y + t^8.95/y + t^8.97/y - t^4.*y - t^5.01*y - t^6.94*y - t^6.97*y - 2*t^6.99*y - t^7.04*y - t^7.94*y - t^7.97*y - 2*t^8.*y - t^8.05*y + t^8.9*y + 2*t^8.92*y + t^8.95*y + t^8.97*y | g2^15*t^2.94 + g2^9*t^2.96 + 2*g2^3*t^2.99 + t^3.04/g2^9 + g2^14*t^3.94 + g2^8*t^3.97 + g2^2*t^3.99 + t^4.02/g2^4 + t^4.04/g2^10 + g2^13*t^4.94 + g2^7*t^4.97 + t^5.02/g2^5 + t^5.05/g2^11 + (g2^26*t^5.45)/g1^3 + (g1^3*t^5.47)/g2^7 + (g1^3*t^5.5)/g2^13 + (g2^8*t^5.52)/g1^3 + g2^30*t^5.87 + g2^24*t^5.9 + 2*g2^18*t^5.92 + 2*g2^12*t^5.95 + 3*g2^6*t^5.97 - 3*t^6. + t^6.03/g2^6 + (g2^25*t^6.45)/g1^3 + (g1^3*t^6.48)/g2^8 + (g1^3*t^6.5)/g2^14 + (g2^7*t^6.53)/g1^3 + g2^29*t^6.87 + 2*g2^23*t^6.9 + 3*g2^17*t^6.93 + 4*g2^11*t^6.95 + 4*g2^5*t^6.98 + t^7./g2 + (2*t^7.03)/g2^7 + t^7.06/g2^13 + (g2^42*t^7.38)/g1^3 + (g2^24*t^7.46)/g1^3 + (g1^3*t^7.48)/g2^9 - (g2^18*t^7.48)/g1^3 + (g1^3*t^7.51)/g2^15 - (g2^12*t^7.51)/g1^3 + (g2^6*t^7.53)/g1^3 + t^7.61/(g1^3*g2^12) + 2*g2^28*t^7.88 + 3*g2^22*t^7.9 + 3*g2^16*t^7.93 + 4*g2^10*t^7.96 + 4*g2^4*t^7.98 + (3*t^8.01)/g2^2 + (2*t^8.03)/g2^8 + (2*t^8.06)/g2^14 + t^8.09/g2^20 + (g2^41*t^8.38)/g1^3 + g1^3*g2^8*t^8.41 + g1^3*g2^2*t^8.43 + (g2^29*t^8.43)/g1^3 + (g1^3*t^8.46)/g2^4 + (g2^23*t^8.46)/g1^3 + (g1^3*t^8.48)/g2^10 - (g1^3*t^8.54)/g2^22 - (g1^3*t^8.56)/g2^28 - t^8.59/(g1^3*g2^7) + g2^45*t^8.81 + g2^39*t^8.83 + 2*g2^33*t^8.86 + 3*g2^27*t^8.88 + 5*g2^21*t^8.91 + 2*g2^9*t^8.96 - 3*g2^3*t^8.99 - t^4./(g2*y) - t^5.01/(g2^2*y) - (g2^14*t^6.94)/y - (g2^8*t^6.97)/y - (2*g2^2*t^6.99)/y - t^7.04/(g2^10*y) - (g2^13*t^7.94)/y - (g2^7*t^7.97)/y - (2*g2*t^8.)/y - t^8.05/(g2^11*y) + (g2^24*t^8.9)/y + (2*g2^18*t^8.92)/y + (g2^12*t^8.95)/y + (g2^6*t^8.97)/y - (t^4.*y)/g2 - (t^5.01*y)/g2^2 - g2^14*t^6.94*y - g2^8*t^6.97*y - 2*g2^2*t^6.99*y - (t^7.04*y)/g2^10 - g2^13*t^7.94*y - g2^7*t^7.97*y - 2*g2*t^8.*y - (t^8.05*y)/g2^11 + g2^24*t^8.9*y + 2*g2^18*t^8.92*y + g2^12*t^8.95*y + g2^6*t^8.97*y |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
57384 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}^{3}$ | 1.4533 | 1.6416 | 0.8853 | [X:[1.3316], M:[0.9974], q:[0.4909, 0.5065], qb:[0.5013, 0.4961], phi:[0.3342]] | t^2.961 + t^2.977 + t^2.992 + t^3.008 + t^3.023 + t^3.964 + t^3.979 + t^3.995 + t^4.01 + t^4.026 + t^4.966 + t^4.982 + t^5.013 + t^5.029 + t^5.468 + t^5.483 + t^5.498 + t^5.515 + t^5.922 + t^5.938 + t^5.953 + 2*t^5.969 + 2*t^5.984 - 2*t^6. - t^4.003/y - t^5.005/y - t^4.003*y - t^5.005*y | detail |