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 |
---|---|---|---|---|---|---|---|---|---|
60057 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ | 1.3916 | 1.5629 | 0.8904 | [X:[1.4196], M:[0.7098, 1.0313], q:[0.4316, 0.7218], qb:[0.5684, 0.5371], phi:[0.2902]] | [X:[[0, 2]], M:[[0, 1], [0, -7]], q:[[-1, 7], [-1, 6]], qb:[[1, -7], [1, 0]], phi:[[0, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }X_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{6}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$ | ${}$ | -3 | t^2.13 + t^2.61 + t^3. + t^3.09 + 2*t^3.78 + t^3.87 + 2*t^4.26 + 2*t^4.65 + 3*t^4.74 + 2*t^5.22 + t^5.52 + 2*t^5.61 + t^5.63 + t^5.71 + t^5.8 + t^5.89 + t^5.91 - 3*t^6. + t^6.19 + 4*t^6.39 + t^6.48 + 3*t^6.5 + t^6.67 + t^6.76 + 3*t^6.78 + 2*t^6.87 - t^7.15 + 3*t^7.26 + 5*t^7.35 + 2*t^7.37 + t^7.45 + t^7.54 + 3*t^7.55 + t^7.63 + 4*t^7.65 + t^7.73 + 3*t^7.74 - t^7.75 + 3*t^7.84 - 2*t^7.85 - 2*t^8.02 + 2*t^8.04 - t^8.12 - 2*t^8.13 + 2*t^8.22 + 2*t^8.24 + 2*t^8.32 + t^8.41 + 4*t^8.42 + t^8.5 + 10*t^8.52 + t^8.61 + t^8.63 + t^8.71 - 2*t^8.72 + t^8.8 - t^8.89 - t^8.99 + t^8.61/y^2 - t^3.87/y - t^4.74/y - t^6./y - t^6.48/y - (2*t^6.87)/y - t^6.96/y - t^7.35/y - t^7.65/y - t^7.84/y + t^8.22/y - (2*t^8.52)/y - t^8.61/y + t^8.71/y + (2*t^8.91)/y - t^3.87*y - t^4.74*y - t^6.*y - t^6.48*y - 2*t^6.87*y - t^6.96*y - t^7.35*y - t^7.65*y - t^7.84*y + t^8.22*y - 2*t^8.52*y - t^8.61*y + t^8.71*y + 2*t^8.91*y + t^8.61*y^2 | g2*t^2.13 + t^2.61/g2^3 + t^3. + t^3.09/g2^7 + 2*g2^6*t^3.78 + t^3.87/g2 + 2*g2^2*t^4.26 + 2*g2^5*t^4.65 + (3*t^4.74)/g2^2 + (2*t^5.22)/g2^6 + g2^4*t^5.52 + (2*t^5.61)/g2^3 + (g2^19*t^5.63)/g1^3 + t^5.71/g2^10 + (g1^3*t^5.8)/g2^8 + (g1^3*t^5.89)/g2^15 + g2^7*t^5.91 - 3*t^6. + t^6.19/g2^14 + 4*g2^3*t^6.39 + t^6.48/g2^4 + (3*g2^18*t^6.5)/g1^3 + (g1^3*t^6.67)/g2^9 + (g1^3*t^6.76)/g2^16 + 3*g2^6*t^6.78 + (2*t^6.87)/g2 - (g1^3*t^7.15)/g2^13 + 3*g2^2*t^7.26 + (5*t^7.35)/g2^5 + (2*g2^17*t^7.37)/g1^3 + (g1^3*t^7.45)/g2^3 + (g1^3*t^7.54)/g2^10 + 3*g2^12*t^7.55 + (g1^3*t^7.63)/g2^17 + 4*g2^5*t^7.65 + (g1^3*t^7.73)/g2^24 + (3*t^7.74)/g2^2 - (g2^20*t^7.75)/g1^3 + (3*t^7.84)/g2^9 - (2*g2^13*t^7.85)/g1^3 - (2*g1^3*t^8.02)/g2^14 + 2*g2^8*t^8.04 - (g1^3*t^8.12)/g2^21 - 2*g2*t^8.13 + (2*t^8.22)/g2^6 + (2*g2^16*t^8.24)/g1^3 + (2*t^8.32)/g2^13 + (g1^3*t^8.41)/g2^11 + 4*g2^11*t^8.42 + (g1^3*t^8.5)/g2^18 + 10*g2^4*t^8.52 + t^8.61/g2^3 + (g2^19*t^8.63)/g1^3 + t^8.71/g2^10 - (2*g2^12*t^8.72)/g1^3 + t^8.8/g2^17 - (g1^3*t^8.89)/g2^15 - (g1^3*t^8.99)/g2^22 + t^8.61/(g2^3*y^2) - t^3.87/(g2*y) - t^4.74/(g2^2*y) - t^6./y - t^6.48/(g2^4*y) - (2*t^6.87)/(g2*y) - t^6.96/(g2^8*y) - t^7.35/(g2^5*y) - (g2^5*t^7.65)/y - t^7.84/(g2^9*y) + t^8.22/(g2^6*y) - (2*g2^4*t^8.52)/y - t^8.61/(g2^3*y) + t^8.71/(g2^10*y) + (2*g2^7*t^8.91)/y - (t^3.87*y)/g2 - (t^4.74*y)/g2^2 - t^6.*y - (t^6.48*y)/g2^4 - (2*t^6.87*y)/g2 - (t^6.96*y)/g2^8 - (t^7.35*y)/g2^5 - g2^5*t^7.65*y - (t^7.84*y)/g2^9 + (t^8.22*y)/g2^6 - 2*g2^4*t^8.52*y - (t^8.61*y)/g2^3 + (t^8.71*y)/g2^10 + 2*g2^7*t^8.91*y + (t^8.61*y^2)/g2^3 |
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 |
---|
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 |
---|
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 |
---|
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 |
---|---|---|---|---|---|---|---|---|---|
57490 | SU3adj1nf2 | ${}M_{1}\phi_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }q_{1}^{2}\tilde{q}_{1}^{2}$ | 1.3969 | 1.5761 | 0.8863 | [X:[1.4051], M:[0.7026], q:[0.4166, 0.714], qb:[0.5834, 0.5013], phi:[0.2974]] | t^2.11 + t^2.68 + t^2.75 + t^3. + 2*t^3.65 + t^3.89 + 2*t^4.22 + 2*t^4.54 + 3*t^4.78 + t^4.86 + t^5.35 + 2*t^5.43 + t^5.51 + t^5.53 + t^5.65 + 2*t^5.68 + 2*t^5.75 + t^5.9 - 3*t^6. - t^3.89/y - t^4.78/y - t^6./y - t^3.89*y - t^4.78*y - t^6.*y | detail |