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 |
|---|---|---|---|---|---|---|---|---|---|
| 2983 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{4}M_{6}$ | 0.5626 | 0.697 | 0.8071 | [X:[1.5707], M:[0.4293, 1.2878, 0.7122, 1.0049, 0.9951, 0.9951], q:[0.9268, 0.6439], qb:[0.361, 0.3512], phi:[0.4293]] | [X:[[2]], M:[[-2], [-6], [6], [-14], [14], [14]], q:[[5], [-3]], qb:[[-11], [17]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{6}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }X_{1}$, ${ }M_{3}M_{5}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | t^2.137 + t^2.576 + 2*t^2.985 + t^3.395 + t^3.424 + t^3.454 + t^3.834 + t^3.863 + t^4.273 + 2*t^4.712 + 2*t^5.122 + t^5.151 + t^5.532 + 2*t^5.561 + 4*t^5.971 - t^6. + 2*t^6.38 + 2*t^6.41 + t^6.439 + t^6.79 + 2*t^6.819 + 2*t^6.849 - t^6.878 + t^6.907 + t^7.229 + 2*t^7.258 + t^7.288 + 2*t^7.668 + 3*t^7.698 + 4*t^8.107 - t^8.137 - t^8.166 + 2*t^8.517 + 3*t^8.546 - 2*t^8.576 + t^8.927 + 5*t^8.956 - 3*t^8.985 - t^4.288/y - t^6.863/y - t^7.273/y + t^7.302/y + (2*t^7.712)/y + (2*t^8.122)/y + t^8.532/y + (3*t^8.561)/y + t^8.59/y + (3*t^8.971)/y - t^4.288*y - t^6.863*y - t^7.273*y + t^7.302*y + 2*t^7.712*y + 2*t^8.122*y + t^8.532*y + 3*t^8.561*y + t^8.59*y + 3*t^8.971*y | g1^6*t^2.137 + t^2.576/g1^4 + 2*g1^14*t^2.985 + g1^32*t^3.395 + g1^4*t^3.424 + t^3.454/g1^24 + g1^22*t^3.834 + t^3.863/g1^6 + g1^12*t^4.273 + 2*g1^2*t^4.712 + 2*g1^20*t^5.122 + t^5.151/g1^8 + g1^38*t^5.532 + 2*g1^10*t^5.561 + 4*g1^28*t^5.971 - t^6. + 2*g1^46*t^6.38 + 2*g1^18*t^6.41 + t^6.439/g1^10 + g1^64*t^6.79 + 2*g1^36*t^6.819 + 2*g1^8*t^6.849 - t^6.878/g1^20 + t^6.907/g1^48 + g1^54*t^7.229 + 2*g1^26*t^7.258 + t^7.288/g1^2 + 2*g1^44*t^7.668 + 3*g1^16*t^7.698 + 4*g1^34*t^8.107 - g1^6*t^8.137 - t^8.166/g1^22 + 2*g1^52*t^8.517 + 3*g1^24*t^8.546 - (2*t^8.576)/g1^4 + g1^70*t^8.927 + 5*g1^42*t^8.956 - 3*g1^14*t^8.985 - t^4.288/(g1^2*y) - t^6.863/(g1^6*y) - (g1^12*t^7.273)/y + t^7.302/(g1^16*y) + (2*g1^2*t^7.712)/y + (2*g1^20*t^8.122)/y + (g1^38*t^8.532)/y + (3*g1^10*t^8.561)/y + t^8.59/(g1^18*y) + (3*g1^28*t^8.971)/y - (t^4.288*y)/g1^2 - (t^6.863*y)/g1^6 - g1^12*t^7.273*y + (t^7.302*y)/g1^16 + 2*g1^2*t^7.712*y + 2*g1^20*t^8.122*y + g1^38*t^8.532*y + 3*g1^10*t^8.561*y + (t^8.59*y)/g1^18 + 3*g1^28*t^8.971*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 |
|---|---|---|---|---|---|---|---|---|
| 3592 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{4}M_{6}$ + ${ }M_{7}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.5751 | 0.718 | 0.801 | [X:[1.5714], M:[0.4286, 1.2858, 0.7142, 1.0002, 0.9998, 0.9998, 0.8572], q:[0.9285, 0.6429], qb:[0.3573, 0.3569], phi:[0.4286]] | t^2.143 + 2*t^2.572 + 2*t^2.999 + t^3.427 + t^3.43 + t^3.856 + t^3.857 + t^4.285 + 3*t^4.714 + 2*t^5.142 + 3*t^5.143 + t^5.57 + 3*t^5.571 + 5*t^5.999 - 2*t^6. - t^4.286/y - t^4.286*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 1945 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ | 0.563 | 0.6963 | 0.8086 | [X:[1.5736], M:[0.4264, 1.2792, 0.7208, 0.9848, 1.0152], q:[0.934, 0.6396], qb:[0.3452, 0.3756], phi:[0.4264]] | t^2.162 + t^2.558 + t^2.954 + t^3.046 + t^3.35 + t^3.442 + t^3.533 + t^3.838 + t^3.929 + t^4.325 + 2*t^4.721 + 2*t^5.117 + t^5.208 + t^5.513 + t^5.604 + t^5.695 + t^5.909 - t^4.279/y - t^4.279*y | detail |